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JPS6322257B2 - - Google Patents
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JPS6322257B2 - - Google Patents

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Publication number
JPS6322257B2
JPS6322257B2 JP15682280A JP15682280A JPS6322257B2 JP S6322257 B2 JPS6322257 B2 JP S6322257B2 JP 15682280 A JP15682280 A JP 15682280A JP 15682280 A JP15682280 A JP 15682280A JP S6322257 B2 JPS6322257 B2 JP S6322257B2
Authority
JP
Japan
Prior art keywords
change
current
counter electrode
coated metal
circuit
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP15682280A
Other languages
Japanese (ja)
Other versions
JPS5780551A (en
Inventor
Takashi Yamamoto
Hiroshi Amako
Mitsuyuki Oda
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Paint Co Ltd
Original Assignee
Nippon Paint Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Paint Co Ltd filed Critical Nippon Paint Co Ltd
Priority to JP15682280A priority Critical patent/JPS5780551A/en
Publication of JPS5780551A publication Critical patent/JPS5780551A/en
Publication of JPS6322257B2 publication Critical patent/JPS6322257B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N17/00Investigating resistance of materials to the weather, to corrosion, or to light
    • G01N17/02Electrochemical measuring systems for weathering, corrosion or corrosion-protection measurement

Landscapes

  • Life Sciences & Earth Sciences (AREA)
  • Biodiversity & Conservation Biology (AREA)
  • Ecology (AREA)
  • Environmental & Geological Engineering (AREA)
  • Environmental Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Testing Resistance To Weather, Investigating Materials By Mechanical Methods (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は塗膜等の被膜を有する塗装金属の塗膜
下金属面の分極特性を測定する方法及びその装置
に関するものである。 一般に塗装された金属は必ず腐食される。すな
わち、塗膜に浸透した水、酸素等の腐食媒体は塗
膜下の金属面に達して、電気化学的反応に供す
る。従つて塗膜の種類、金属の種類、金属表面の
種類、塗装金属が置かれる環境等々によりその反
応速度、反応種類は多種多様を呈することにな
る。従来より塗装金属の耐食性を判定する方法と
しては、目視にたよることが多く、塗装金属面に
認められるサビの発生時間、サビの面積、等々の
大小をもつて実用的判定法とされる事が多い。 ところが、より防食性能の良い塗料の開発、よ
り良い塗装用金属、あるいは腐食による事故予
見、塗装の塗り替え時期の判定等々は工業的に極
めて要望の強い項目でもある。これらを満足しよ
うとするには従来の上記目視判定法等にたよるこ
とは極めて大きなキケンが伴う。何故なら、塗装
金属でサビが観察された時点を考えるならば、塗
膜欠陥が生じ(例えば塗膜が破壊され)塗膜の下
の金属の腐食反応生成物(鉄分の赤サビ等は主に
水酸化鉄)が、その欠陥を介して塗膜表面に出て
いる状態を示しているにすぎず、実際には、それ
以前に腐食が進行していることになる。にもかか
わらず、塗膜表面に出てくるサビを判定しても工
業的に有効な方法であるか疑問となる。例えば今
塗膜下金属に孔が開く腐食形態を考えると、必ず
しも塗膜が破壊される以前に塗膜の下の金属の孔
開き時間が早い場合も多い。特に昨今の様に厚膜
型の塗装あるいはライニング等の施行方式にこの
ような例がみられる。 一方、塗膜の下の金属の腐食状況を判定する外
に、塗膜自身の劣化速度を把握することも重要で
ある。このため従来、剥離膜でのイオン透過性、
水蒸気透過性、酸素透過性、更には誘電損失率
等々の測定が行われている。ところが、これらの
値は実際の塗装金属の腐食・防食性能とは必ずし
も対応しない。したがつて、好ましくは実用の塗
装された状態での塗膜の特性を測定することであ
り、そして、これらの得られた(上記の膜特性)
値と、塗膜の下の金属の腐食反応とを結びつける
ことにより、工業的価値がある塗装鋼板の耐食性
評価が可能であると思われる。 上記の現状を鑑み、本発明者は鋭意努力して、
その評価法の研究開発に取り組んできた。すなわ
ち、本発明者等は、例えば日本特許No.960239号の
内容を更により有効なものとすべき考えで取組ん
できたものである。すなわち、上記特許はある1
つの速度で塗装金属を分極したときの電位と電流
との関係において、塗膜抵抗成分のみ除いた分を
検出するものである。すなわち、電位―電流の関
係において、塗膜の抵抗値は一定であるとみなし
ている。 ところが全ての塗装された塗膜の電気抵抗は分
極の大きさにより不変であるとは言い難い塗膜も
存在することを見出した。この事実に基づいて本
発明は高抵抗塗膜を塗装した鋼板の腐食塗装鋼板
における塗膜下鋼表面近傍の分極特性で測定する
こと、並びに、この鋼表面近傍の分極特性を利用
して、塗装鋼板の耐食性評価が可能かどうかを検
討することを目的とするものである。 本発明を完成に導いた第1の特徴は、従来、あ
る1つの速度(定電位電解法では、ある1つの速
度で試料の電位を増加、又は減少させる。一方定
電流法ではある1つの速度で電流を印加してゆ
く)で分極してゆくが、本発明は2つ以上の異な
つた速度で分極すること。第2の特徴は、分極速
度kとすると、kを変えても塗膜のみではv/k
(vは試料への加電圧…定電流電解法の場合)又
はi/k(iは試料への加電流…定電位電解法の
場合)の値はkに依存しないが、塗装金属では依
存することを見出した。第3の特徴は、従来の方
法により評価された結果、耐食性が劣る(例え
ば、ブリスターが発生している、サビが認められ
る、防錆顔料の効果が発揮されていない、あるい
は、一見塗膜状態は正常であつても塗膜の下の金
属に孔が貫通している等々の状況)と判定される
塗装金属では、上記第2の特徴の塗膜のみの挙動
になる。すなわち、kを変えてもv/kの値はk
に依存しない。第4の特徴は、正常な塗装金属は
kに依存するが、塗装金属が劣化してゆくと、k
に依存しなくなつてゆき、この依存性の追跡よ
り、塗装金属の劣化速度を知ることができ、塗装
金属の劣化予測、塗装金属のモニタニングに応用
可能である。 詳しくは、第1番目の発明は、2つ以上の異な
つた速度を有する直線状に変化する電圧を塗装金
属に印加した時の電流の差を測定する方法とし
て、 塗膜を有する塗装金属と対極とを溶液中に浸漬
し、該塗装金属と対極面に大略元の非通電状態に
戻すに十分な1定時間以上の非通電間隔をおい
て、各通電時間毎に夫々全く異なる電圧変化率を
もつて正又は負に直線的に変化する種々の直流電
圧又は電流のいずれかを断続的に印加し、上記塗
装金属と対極間に流れる上記各通電時間中に流れ
る夫々の電解電流又は電圧のいづれかの単位時間
毎の時間変化を上記の夫々対応する通電時間の電
圧変化率で割り算をして各除値を求め、該割り算
値のいづれか一つの基準値とし該基準値と他の割
り算値とその差を取り出し、その差と上記直流電
圧の印加時間との関係を求めることを特徴とする
塗装金属における塗膜下金属面の外部分極特性を
測定せんとするものである。 そして、第2番目の発明は、2つ以上の異なつ
た速度を有する直線状に変化する電流を塗装金属
に印加した時の電位の差を測定する方法であり、
塗装金属と対極とを溶液に浸漬し、該塗装金属と
対極的に、少なくとも1分間以上の間隔をおい
て、2つ以上の異なつた速度をもつて正又は負に
直線的に変化する直流電流を印加し、上記塗装金
属の2つ以上の電極電位の時間変化を、上記の
各々の速度で割り算をし、その差と分極時間との
関係を測定することを特徴とする塗装金属におけ
る塗膜下金属面の外部分極特性を測定せんとする
ものである。 さらに、第3番目の発明は、少なくとも塗装金
属と対極とを溶液中に浸漬してなる測定セルと、
上記塗装金属と対極間の電極電位差を検出する手
段と、この電極電位差と同一の略電位を上記塗装
金属と対極間に印加し、保持する手段と、2つ以
上の異なつた速度を有し、かつ直線状に変化、か
つ正又は負に変化させうる直流電位発生して上記
塗装金属と対極間に印加する手段と、該直流電位
発生手段を1分間以上の間隔をもつて上記直流電
流を上記塗装金属と対極間に印加させうる印加手
段と、上記塗装金属と対極間に流れる電解電流変
化を測定する装置と、該測定された2つ以上の値
を上記の各々の速度で、割り算、かつ記憶する装
置と、該異る正電時間における互に対応する時間
毎に割り算された2つ以上の値の差を取り出し、
その差と通電時間との関係を記録する装置とを備
えることを特徴とする装置を新規に提案するもの
である。 また、第4番目の発明は、少なくとも、塗装金
属と対極とを溶液に浸漬してなる測定セルと、2
つ以上の異なつた速度を有し、かつ直線状に変化
かつ、正又は負に変化させうる直流電流発生手段
と、該直流電流発生手段を1分間以上の間隔をも
つて動作させうる制御手段と、上記塗装金属の電
位変化を測定する装置と、該測定された2つ以上
の値を上記各々の速度で割り算、かつ記憶する装
置と、該割り算された2つ以上の値の差を取り出
し、その差と分極時間との関係を記録する装置と
を備えることにより、2つ以上の異なつた印加電
流速度で塗装金属を分極したときの、2つ以上の
電解電位の差を、測定する装置を提供しようとす
るものである。 以上、本発明は従来の定電位電解方法と該方法
に係る装置であるポテンシヨスタツト、並びに従
来の定電流電解方法と該方法に係る装置であるガ
ルバノスタツトに極めて類似している様に思われ
がちであるが、本発明の特徴は従来のように任意
の時間に、あるいは一定間隔を置いた時間にある
所定の速度で試料に加電圧、並びに加電流したと
きの、電流変化並びに電圧変化を測定し、試料と
溶液との反応速度(腐食速度等)、経時変化等を
求めて試料をより耐食性の良好な物質にする、あ
るいはその試料の寿命を予測して腐食による事故
を抑制するため予じめ試料を交換しようとする場
合に用いようとするものではない。すなわち、本
発明は従来のものとその目的は同一であつても、
得られる測定値、得ようとする方法、その方法に
用いる装置が極めて新規である。従来の方法、装
置の意味するところのその第1は2つ以上の異な
る速度で金属を分極することは公知であり、該速
度依存性で金属の性能、性質を判定しようと試み
られていることも公知である。言い換えれば、同
一の1個又は複数の試料でもつて異なつた速度で
分極したとき、そのときの分極の差は各々の分極
速度での試料と腐食との反応性の差であり、あき
らかに各々の分極時の試料が異なつた状態を示し
た結果の差である。第2は、一定間隔又はある時
間置いて、2回以上分極したときの差も時間経過
により、どの程度試料が変化したかの情報を求め
ようとするものであり、上記第2の意味と同じで
ある。第3は、上記の第1と第2との組合せが実
施される場合もあろうが、上記と同じように、試
料の変化量、あるいはその変化内容を測定しよう
とするものである。 ところが本発明は後記する実施例でその詳細を
示すが、定電位法にあつては得られる電解電流を
印加電圧の速度で割り算をして、かつ、2つ以上
の異なつた印加電圧速度をもつて同様に各々の速
度で得られる電解電流を各々の速度でもつて割り
算をし、その差と電圧を印加する時間とを相関さ
せ、塗膜の下の金属表面の情報を得ようとするも
のである。一方、定電流法にあつても、同様であ
り、上記では得られる値が電解電流であるが、該
方法では、それが電位であることのみ異なつてい
ることである。すなわち、本発明は、塗装金属を
分極することにより得られる電流、並びに電位を
分極速度で割り算をすることにより塗膜に起因す
る値を除くことにあり、その結果として塗膜下金
属表面近傍、いわゆる塗膜下金属の腐食・防食反
応の情報が得られることにある。 次に本発明の内、定電位電解法すなわち、第1
の発明の基本思想を第1図に用いて説明する。第
1図は定電位法に係るもので、第1図イにおい
て、1は測定セルで、塗装金属W、基準電極R、
対極Cを備え、該CとRの間に高入力抵抗変換器
AMPIと演算器AMP2を介在させると共に上記
Wに電流計Aを接続する一方、電圧計V、加電圧
走査発生器Vtおよび直流電圧発生・保持機構―
Voを備える。第1図ロは実際の回路構成を示す
もので、図中、1は測定セルで、水溶液腐食液有
機溶剤あるいはそれらの混合物等々の溶液(一般
に用いられる電解質液でなくてもよい。)中に対
極Cと塗装金属Wを浸漬してなる。対極C、塗装
金属Wは溶液を介して、2aの第1直流電圧電
源、3aの第2直流電圧電源、4aの電流計及び
5aのスイツチのON状態により閉回路を構成し
ている。一方、電圧計6aは対極C及び塗装金属
Wに接続されている。 7aは割り算回路で、上記電流計4a及び引き
算回路8aに接続されている。一方、9a,10
aは記憶回路で前者の記憶回路9aは、上記C―
W間に流れる電流の時間変化をいつたん記憶する
もので、後者の記憶回路、10aは上記割り算回
路7aで、上記C―W間に流れる電流の時間変化
を、上記第1直流電源2aの印加速度で割り算さ
れた値を記憶する回路であり、必ずしも前者の記
憶回路9aでいつたん記憶する必要性はないの
で、該記憶回路9aを設けないで以下にその動作
の基本を記する。 いま、スイツチ5aを開きOFF状態にすると
電圧計6aの値は、C―W間の電位差、すなわ
ち、溶液中での対極C及び塗装金属Wの各々の自
然電極電位の差となる。これをVoとすると、こ
のVoと極性の異なる同一の電圧―Voを第2直流
電源3aの大きさとなる様に、第2直流電圧電源
3aを調整する。次いでスイツチ5aをONにす
るとC―W間にはC―W間の電位差Voと逆の電
位差―Voが印加されるため、電流計4aの電流
は略ゼロとなる。(この状態を以下塗装金属の自
然電極電位で電解した状態と称することにする)。
この状態にした後、上記の第1直流電圧電源2a
を動作させ、k1なる印加速度で電圧を直線的に変
化させると同時に、上記の割り算回路7a記憶回
路10aを動作させる。以上の動作により、C―
W間に電流が流れ、電流計4aを介して、電流の
時間変化はk1で常に割り算され、その結果の値は
時間変化として記憶回路10aに記憶されてゆ
く。次いで所定の時間(以下分極時間と称する)
まで分極した後、スイツチ5aをOFF、及び第
1、第2直流電圧電源2a,3a並びに割り算回
路7aを元の状態にもどすと同時に、上記の動作
で得られた値を、記憶回路10aで記憶してお
く。以上の操作により、塗装金属は、自然の状態
(無電解状態)にもどつたことになり、この状態
で1分間以上保ち、再び第2直流電圧電源3aに
より上記と同様、塗装金属の自然電極電位で電解
し、電流計4aの値を略ゼロに設定する。次いで
第1直流電源2aにより、今度はk2なる印加電圧
速度で直線的にC―W間に直流電圧を印加してゆ
く。その時の電解電流を電流計4aを介して、割
り算回路7aに入力し、その値を常にk2で割り算
し、その値の時間変化を記憶回路10aに記憶し
てゆき、所定の分極時間まで分極する。ついで上
記したk1で割り算された値と上記k2で割り算した
値との差を引き算回路8aで分極経過時間を同期
させながら演算し、その結果を測定する。あるい
はまた、k2で割り算されてゆく時間変化の値を記
憶させないで、先にk1で割り算された値の時間変
化とk2で割り算されてゆく値の経過時間(分極時
間)とを同期させながら引き算回路8aで演算
し、その値を求めても上記と同一となる。すなわ
ち、先に分極した値のみを記憶させ、次に分極さ
れる値は、記憶しないで行う方式でも同じ値とな
る。 次に、本発明の内、定電流法、すなわち、第2
の発明の基本思想を第2図を用いて説明する。 第2図イにおいて、1は測定セルで、塗装金属
W、基準電極R、対極Cを備え、該CとWの間に
高入力抵抗変換器AMPIと演算器AMP2を介在
させる一方、RとWの間に増巾器AMP1′と電圧
計V′を介在させ、かつWに可変抵抗r1を介して電
流計A′を接続すると共に加電圧走査発生器Vx′を
備える。第2図ロは実際の回路構成を示すもの
で、第1図ロと異なつているのは、第1図の第1
直流電圧電源2aが第2図では直流電流電源2′
aに、同様に、第2直流電流電源3aが第2図で
はゼロ電流器3′aに、更に割り算回路7a、記
憶回路10a、引き算回路8aは夫々電流の時間
変化を演算、記憶するものであるのを、第2図の
割り算回路7a、記憶回路10a、引き算回路8
aは電位を演算記憶するものにしたのみであり、
そのために第2図では、電圧計6aの出力を割り
算回路7aに接続しているにすぎない。従つて前
記した第1図の基本的測定動作と同じである。但
し、第1図では塗装金属を自然電極電位状態で電
解し、C―W間の電流を略ゼロにするため、第2
直流電位電源の大きさを―Voにしたが、第2図
では、C―W間の電流をゼロにするため、―Ioを
印加してゼロにするゼロ電流器3′aを用いた。
以上の構成により、第1図ではk1あるいはk2なる
加電圧速度で分極したが、第2図ではk′1,k′2
る加電流速度で分極するにすぎず、基本的動作は
第1図で説明した内容と類似するので説明は省略
する。 次に第1番目の発明を実施する装置である第3
番目の発明の実施例について詳細に説明する。 前記した、対極C自身の電極電位は溶液中で安
定かつ対極Cと塗装金属Wとの間に電流が流れて
も対極C自身の電位は安定で変化しにくい事が必
要であり、通常、塗装金属Wを測定しようとする
場合、例えば対極Cは銀―塩化銀電極あるいはカ
ロメル電極等を使用してもかまわない。すなわち
塗膜の電気抵抗は極めて大きく、無塗装金属に比
べて電解電流は極めて小さく、対極自身の分極に
よる影響は少ない。しかし、より精度の高い測定
を行つて塗膜下金属表面の腐食・防食反応を検出
するには、対極自身のより安定化が望ましい場合
も必要となる。そこで、以下の実施例は、少なく
とも対極Cは単に塗装金属Wへの電流の出入りを
受けとめる電極としての役目のみとし、かつ上記
した対極自身の分極による影響が測定値に加わら
ないために、前記した測定セルに基準電極を備
え、該基準電極の信号を用いた。すなわち、第1
番目の発明には、対極Cと塗装金属Wとの電極電
位差によつて生ずる誤差電流を予じめ略零に設定
するような測定手段を備える一方、第2番目の発
明には、対極Cと塗装金属Wとの電極電位差が安
定して測定できる検出手段を備えて、少なくとも
上記した対極自身の分極の影響を極力抑制して、
上記塗装金属の分極電流を測定信号とするもので
ある。 次に、第3図は、本発明に係る塗装金属の塗膜
下金属面の外部分極特性を定電位電解法により自
動的に測定する装置のブロツク図で、第4図は、
その配線図である。以下、第3図と第4図を対比
しながら、操作順及びブロツク毎に説明する。 先ず、測定セル1は、無機物、有機物あるいは
該混合物からなる皮膜、塗膜を表面に有する金属
の塗装金属板W、及びカロメル電極銀―塩化銀電
極等安定な電極電位を示す基準電極R、並びに白
金等の腐食されにくい無塗装金属からなる対極C
とを、3%NaClの腐食液に浸漬してなり、塗装
金属板Wの電極電位及び電解電流を1分間以上の
間隔をもつて2回測定、演算し、その差を測定時
間を同期させた上で取り出し、それをもつて塗膜
下金属表面の分極特性が測定可能となつている。 次に、電極電位測定手段2は、塗装金属W―基
準電極R間の抵抗(浸漬液中の塗膜の電気抵抗+
液抵抗+対極表面及び塗膜下金属表面の分極抵抗
と称される界面抵抗からなる抵抗)より充分高い
(通常1013Ω以上)入力抵抗を有する高入力抵抗
変換器3を介して、上記基準電極Rに接続され、
かつ他端が接地された電圧計であり、下記する印
加電圧によつて生じる電解電流が極力入力されな
いようにして、塗装金属Wの電極電位を測定して
いる。詳しくは、上記変換器3の出力が、抵抗器
R1を介して接地され、該抵抗器R1の両端の電位
差を測定するように直流増巾器AMPと抵抗器R2
を並列に接続し、一方は上記変換器3の出力側に
他端は上記電圧計の出力信号として用いるもので
あり、抵抗器R1とR2との比により増巾度を変え
られるようになつている。 さらに、溶液中での塗装金属Wの自然電極電位
で電解できるようにする測定準備手段4は、上記
電極電位測定手段2に一方が接続される一方他端
が接地されるサーボ機構5と、補償信号供給手段
6とスイツチ7、及び第1演算機8とを備える。
さらに、第4図を用いて詳細に説明すれば、まず
演算器8の入力側は、上記高入力抵抗変換器3
と、補償信号供給手段6のポテンシヨメータP1
とに接続すると共に、該手段の出力側はスイツチ
7の閉状態(c―d間が接続)を介して接地され
ている。そして演算器8の出力側は上記対極cに
接続され、上記高入力抵抗変換器3の出力(電極
電位信号)aと、上記補償信号供給手段6の出力
(補償電位信号)bとを演算し、上記塗装金属W
と対極c間の電極電位差によつて生じる誤差電流
を略零にしている。 さらにサーボ機構5は、比較器9とサーボモー
タ10と比較信号供給手段11とからなつて負帰
還回路を構成している。詳しくは比較器9の入力
側は、上記した電極電位測定手段2の直流増巾器
AMPの出力に接続するとともに、比較信号供給
手段11に接続する一方、出力側は常開接点L1
を介して上記サーボモータ10に接続され、上記
電極電位測定手段2の出力(電位信号)Vaと上
記比較信号供給手段11の出力(比較信号)―
Vaとを比較して、その差の信号である出力を、
上記常開接点L1をON状態(閉)にすることによ
り、上記サーボモータ10に入力し、該モータを
駆動する。該サーボモータ10の駆動に連動され
ているのが、上記した補償信号供給手段6のポテ
ンシヨメータP1と、上記した比較信号供給手段
11のポテンシヨメータP2であり、詳しくは、 補償信号供給手段6は、ポテンシヨメータP1
と直流電源E1、及び分配抵抗R3,R4とを並列に
接続してなり、上記分配抵抗R3,R4の接続点か
ら上記したように上記スイツチ7の閉状態(c―
d間を接続)を介して接地される一方、ポテンシ
ヨメータP1を介して上記第1演算器8に接続さ
れており、該手段6の出力電圧(補償信号)a
は、上記サーボモータ10の駆動により、常に補
償しながら上記第1演算器8に入力するようにな
つている。一方、上記比較信号供給手段11のポ
テンシヨメータP2は、直流電源E2と分配抵抗R5
R6とにより並列的に接続され、該分配抵抗R5
R6の分岐点は接地、及びポテンシヨメータP2
上記した比較器9に接続して比較器信号―Vaを
入力している。そして、常開接点L1をON(閉)
にすることにより、比較器9の入力Vaと―Vaと
が比較され、略その差がゼロになる様、上記した
ポテンシヨメータP2が変位する様、サーボモー
タ10が駆動され、同時に上記した補償信号供給
手段6のポテンシヨメータP1も変位し、上記し
た第1演算器8のa―b間の電位差も略ゼロにな
り、その結果上記したサーボモータ10は駆動停
止状態になる。 以上の構成をもつて、測定の準備が行われ、上
記した第1演算器8の出力は略ゼロとなり、その
結果上記した対極cと塗装金属Wとの間の電解電
流は略ゼロとなる。この準備状態が前記した塗装
金属Wの自然電極電位で電解した状態である。以
下、この状態を第1回準備状態と称する。 次に、上記塗装金属Wに正又は負の直線的勾配
を有する直流電圧を印加する電源12は、ポテン
シヨメータP3と直流電源Eと分配抵抗R7,R8
並列して接続してなり、出力例であるポテンシヨ
メータP3は上記したスイツチ7の開接点側e、
共通接点cを介して、上記補償信号供給手段6の
分配抵抗R3,R4の分岐点に接続されるようにな
つているとともに、分配抵抗R7,R8の分岐点は
接地されている。以上の構成により、ポテンシヨ
メータP3の変位により、正又は負の勾配の直流
電圧が該直流電圧印加電源12から出力され、上
記したスイツチ7をc―e間に接続すれば、上記
した補償信号供給手段6の出力電圧と重畳して、
第1演算器8の入力b側に入力でき、その結果該
演算器を介して上記対極cには、該重畳した電圧
が印加される。 次いで、塗装金属の分岐によつて流れる電解電
流を測定する装置13は、直流増巾器14と多段
抵抗器15とを備える。詳しくは、直流増巾器1
4は、抵抗器R9と並列して接続され、その入力
側は、上記塗装金属Wに接続されるとともに多段
抵抗器15を介して接地されている。すなわち、
多段抵抗器15は、抵抗器R10〜R13と常閉接点
L2及び常開接点L3〜L5を各々直列に接続すると
ともに全体を並列に接続してなり、上記接点の切
換により適宜適当な電圧降下が得られるように
し、かつ、抵抗器R10〜R13の抵抗値と上記した
抵抗器R9の抵抗値により、上記した直流増巾器
14の出力電圧の増巾度を変えられるようにした
ものである。従つて、上記した対極cを塗装金属
W間に流れる電解電流を電圧に変換して検出して
いる。 次に、上記した第1回準備状態にした後、上記
直流電圧印加電源12の出力は、正又は負の直線
的勾配を有する速度で直流電圧を発生しうるため
に、上記ポテンシヨメータP3は、シンクロナス
モータ16によつて一定速度で変位するようにな
つており、この変位速度kx(V/sec)は、変位
コントロール手段17で制御される。上述のよう
に、上記対極cを用いて塗装金属Wに正又は負の
電位勾配の直流電位(V/sec=kx)を印加する
ようにシンクロナスモータ16を駆動すれば、そ
れに対応する塗装金属Wの電解電流変化が、上記
電解電流測定装置13の上記多段抵抗器15によ
り適当な電圧降下を受けて直流増巾器14に入力
して増巾された後、測定信号として出力される。
該出力電圧は、割り算回路18に入力されて上記
した直流電圧印加電源12の変位速度kxで割り
算される。 詳しくは、割り算回路18は、直流増巾器1
9、多段抵抗器20を備え、かつ、直流増巾器1
9は抵抗器R14と並列に接続され、その入力側は
上記電解電流測定装置13に接続されるととも
に、多段抵抗器20を介して接地されている。ま
た、出力側は、スイツチ21に接続されている。
多段抵抗器20は、抵抗器R15〜R18と常閉接点
L6及び常開接点L7〜L9を各々直列に接続すると
ともに、全体を並列に接続してなり、上記接点の
切換により適宜適当な電圧降下が得られるように
し、かつ、抵抗器R15〜R18の抵抗値と上記抵抗
器R14の抵抗値により、上述した電解電流の変化
を上記変位速度kxで割り算する。すなわち、電
解電流iの時間変化i―tを常にkxで割り、そ
の値を常に上記直流増巾器19の出力とするよう
にしたもので、上記変位速度kxは、上記多段抵
抗器20の適当な抵抗値を設定することにより得
られる。 次に、上記割り算回路18で出力される値の時
間変化は、上記スイツチ21(f―g間に接続)、
及び常開接点L10の閉状態を介して、第1記憶回
路22に記憶される。詳しくは、上述対極Cによ
り塗装金属Wに直流電圧を上述kxなる速度で直
線的に正又は負に印加してゆくときに塗装金属W
に流れる電解電流の時間変化をkxなる値で割り
算し、その結果の時間変化を上記第1記憶回路2
2に記憶される。そして、所定の時間分極した
時、上記常開接点L10を開状態にして記憶を中止
し、測定終了とする。そして、1分間以上、次の
測定まで待機及び各手段回路スイツチを元の状態
にもどすための制御装置33からの信号が第3図
に示す点線を介して送られる。例えば、上記スイ
ツチ7をc―d間の接続に切換え、かつ上記直流
電圧印加電源12の出力電圧を零となるように、
上記ポテンシヨメータP3を上記シンクロナスモ
ータ16を介してスタート状態にもどす。 以上の構成をもつて、上述第1回の準備状態か
ら、上述kxなる印加速度で塗装金属Wが分極で
き、その時の電解電流i―tをkで割算したi―
t/kの値が記憶回路に記憶された状態になる。
これを、以下、第1回測定と称する。なお、上記
第1記憶回路22は、記憶型シンクロスコープ、
あるいは通常のホールド式デジタル電圧計を多数
並列して接続する等々、多くの方法があるので、
詳細は省略する。 次に、上記第1回測定が終了した後、1分間以
上、前述した第1回準備状態までの操作、構成と
同じ事を繰り返し、上記サーボモータ10により
ポテンシヨメータP1,P2が自動的に調整されて、
対極Cと塗装金属Wとの間に流れる電解電流は常
に略ゼロとなる。すなわち、塗装金属の自然電極
電位で電解されている状態となる。以下、これ
を、第2回準備状態と称する。 次に、1分間以上待機した后、上述したように
上記スイツチc―e間に接続して、上記k′xなる
速度で上記シンクロナスモータ16を駆動させ、
上記ポテンシヨメータP3をkxなる速度で変位さ
せると同時に、上記多段抵抗器20の常閉接点
L6を開状態、常開接点L7を閉状態にして、抵抗
器R16が接地される状態にする。更に、上記スイ
ツチ21をf―h間の接続に切換え、かつスイツ
チ24のj―l間に接続し、常開接点L11を閉状
態にして、上記第1記憶回路を同様な第2記憶回
路23に、上述したと同じように電解電流の時間
変化(i′―t)を印加速度(k′x)で割り算され
た値が常に記憶されることになる。この構成をも
つて測定される状態を、以下、第2回測定と称す
る。但し、該第2回測定が上述した第1回測定と
特に異なるのは、上記変位コントロール手段17
で制御される上記ポテンシアメータP3の変位速
度が、k′xになつた事である。そして、所定の時
間まで上記塗装金属Wを分極すれば、上記常開接
点L11を開状態にして、第2記憶回路23の記憶
を中止し、かつ、上記スイツチ7をc―d間の接
続に切換えて、上記直流電圧印加電源12の出力
電圧を零となるように、上記ポテンシヨメータ
P3を上記シンクロナスモータ16によりスター
ト状態にもどす。 以上の構成で、上記記憶回路22及び23には
電位の時間変化(本来この時間変化は、塗装金属
Wに流れる電流の時間変化を所定の値で割り算さ
れた値であるが、前述したように、上記電解電流
測定装置13は、直流電流を直流電圧に変換して
出力されるように本実施例では構成されている。)
が記憶された状態となる。詳しくは、i―t/
kxとi′―t/k′xが記憶されている。 次いで、上記第1記憶回路22、第2記憶回路
23は各常開接点L12,L13を介して、差検出器2
4、記録装置25に夫々接続されている。詳しく
は、差検出器24は、第2演算器26と電圧計2
7で構成され、かつ、第2演算器26の入力は、
上記常開接点L12を介して上記第1記憶回路22
の出力、及び、上記常開接点L13を介して上記第
2記憶回路23に各々接続されるとともに、その
出力は電圧計27を介して接地されている。一
方、該電圧計の出力は、通常のペン書き式レコー
ダー、又はオシロスコープ、シンクロスコープ
等々の上記記録装置25に接続されている。 次に、上記常開接点L12及びL13を閉状態にし
て、上記第1記憶回路22と上記第2記憶回路2
3を同時に作動させ、かつ、時間的に同期させな
がら上記第2演算器26に入力されると、該演算
器26のm―q間の差、詳しくは、上記した第1
記憶回路22に記憶されているi―t/kxと上
記した第2記憶回路23に記憶されているi′―
t/k′xとの差(△i/k)が、上記第2演算器
26で検出され、その出力が、上記電圧計27を
介して、上記記録装置25に記録させてゆけば、
目的とする塗装金属の塗膜下金属面の外部分極特
性が得られる。 一方、スイツチ28をj―n間に接続して常開
接点L14を閉状態にして、上述した第2回測定を
スタートすると同時に、上記した第1記憶回路に
記憶されたi―t/kxを、順次常開接点L12を閉
状態にして、上記第2演算器26に送り込めば、
上記した△i/kが、上記と同様、記録装置25
に記録されることになり、上記第2記憶回路22
は不要となる。但し、2つ以上の上記変位速度
kxの測定を行い、多数のkxの値での各々の差△
i/kxを検出、記録するには適当と言えない。
このためには、第1記憶回路22と第2記憶回路
23をくり返し使用することで可能となる。例え
ば、第1回測定でk1、第2回測定でk2、第3回で
k3、第4回でk4とすると、第1記憶回路にk1、第
2記憶回路にk2での値を各々記憶させ、第3回測
定のときのk3でのi―t/k3を第1記憶回路に記
憶されている。i―t/k1の値を取り除きなが
ら、あるいは、第3回測定前に予じめi―t/k1
の値をゼロにするかを行い、第1記憶回路に記憶
してゆく。そして、第1記憶回路のi―t/k3
第2記憶回路のi―t/k2との差を記録装置で記
録する。次いで、同様に、k2で得られた値をゼロ
にして、k4の値を記憶してゆくように順次切換え
ながら行つても本発明の目的を達することができ
る。あるいは、必要とするkxの数だけの記憶回
路を設けてもよい。又第3図には上記の各々の装
置、回路、接点、スイツチの制御、及び、記憶回
路22,23の同期動作、シンクロナスモータの
スタート、ストツプ、速度制御等々を行わしめる
制御装置33を示しており、少なくとも該制御装
置33の制御信号の接続を点線で示したが、その
動作の基本は上述したので以下省略する。 次に、第2番目の発明を実施する装置である第
4番目の発明の実施例について、詳細に説明す
る。 第5図は、本発明に係る塗装金属の塗膜下金属
面の外部電極特性を定電流電解法により自動的に
測定する装置のブロツク図で、第6図は、その配
線図である。第5図,第6図を対比しながら、並
びに前述した第3図,第4図をも対比しながら、
操作順、及びブロツク毎に説明する。 まず、測定セル1、及び該測定セル1内に溶
液、対極C、塗装金属W、基準電極Rを各々設け
ることは前述(第3図,第4図を用いて実施例を
説明済)した。同様に、高入力抵抗変換器3、ス
イツチ7、第1演算器8、直流電圧印加電源1
2、シンクロナスモータ16、及び変位コントロ
ール手段17は、前述した第3図,第4図との構
成と同じであるので個々の操作及びブロツク毎の
詳細は省略し、特に、上記の内第2番目及び第4
番目の発明に係る部分のみを詳細に説明する。 塗装金属Wは、電流制御用可変抵抗器29を介
して接地、かつ、上記高入力抵抗変換器3に直接
接続され、該高入力抵抗変換器3の出力は、上記
第1演算器8の入力aに接続、かつ、該第1演算
器8の出力は対極Cに接続されている。一方、上
記第1演算器の入力bは上記スイツチ7のc―d
間接続を介して接地されている。すなわち、上記
第1演算器8の入力a―b間には、接地を通じ上
記電流制御用可変抵抗器で閉じられていることに
なり、該第1演算器8の出力はゼロとなる。従つ
て、対極Cと塗装金属Wとの間には電流が流れ
ず、前述した塗装金属Wの自然電極電位で電解し
たことになる。 次いで、上記スイツチをc―e間に接続し、前
述した直流電圧印加電源12のポテンシヨメータ
P3をシンクロナスモータ16の速度を変位コン
トロール手段17を用いて駆動すれば、上記直流
電圧印加電源12の出力電圧が、上記対極C、塗
装金属W間に加わる。ところが、上記した電流制
御用可変抵抗器29が塗装金属Wと接地との間に
接続されているため、上記対極C―塗装金属W間
の電圧印加制御が行われず、上記対極C―塗装金
属W間の電流印加制御となる。すなわち、今、対
極―塗装金属W間に直線的加電流を印加する速度
をk′i(A/sec)、上記直流電圧印加電源12の出
力電圧の直線的電位変化速度k′v(mv/min)、上
記電流制御用可変抵抗器29の電気抵抗値r′(Ω)
とすれば、k′iは次式で表わされる。 k′i=k′v/r′×60×1000 (A/sec) 従つて、上記したポテンシヨメータP3の駆動
速度、並びに上記電流制御用可変抵抗器29の値
を変えることにより、上記対極Cと塗装金属Wと
の間に正又は負の直線的電流変化を与えることが
でき、したがつて、前述した正又は負の直線的電
圧変化を対極C―塗装金属Wに与えるため、上記
直流電圧印加電源12及びシンクロナスモータ1
6変位コントロール手段17を用いたが、同じ手
段を利用できることになり極めて便利と言える。 次に、上記対極C―塗装金属W間に直線的電流
変化を与えたときの上記塗装金属Wの電極電位変
化を追跡するため、基準電極Rと塗装金属Wとの
間に電圧計30が設けられている。詳しくは、上
記基準電極Rは塗装金属W―基準電極R間の抵抗
より充分高い(通常1013Ω)以上)入力抵抗を有
する高入力抵抗変換器31を介して、直流増巾器
32の入力側の1つであるSに接続され、かつ、
該直流増巾器32の他方の入力の1つであるt側
には上記塗装金属Wに接続されている。以上の構
成により、上記対極C―塗装金属W間に電流が印
加されてゆくと、上記基準電極R―上記塗装金属
W間の電位変化は、上記直流増巾器の出力として
検知しうることができる。 次いで、上記電圧計30の出力yは、今第6図
中の点とすると、この点は第5図中の点で
あり、該出力yは前述した割算回路18の入力に
接続される。そして、第5図のスイツチ21、第
1記憶回路22、第2記憶回路23、差検出器2
4、記録装置の各々の構成及び接続、動作内容
は、前述した第3図及び第4図を用いて説明した
ことと同じである。すなわち、第5図、第6図の
点は、第3図,第4図の点と同じである。第
3図,第4図を用いて実施例を説明した内容は塗
装金属Wに「電圧を与え、その応答信号として電
流を検知し、該電流を電圧に変換し」、該電圧を
上記第3図,第4図の点に送り、割算及び2つ
の信号の差を検出、記録するものであり、第5
図,第6図を用いて実施例を説明した内容は、塗
装金属Wに「電流を与え、その応答信号として電
圧を検知し」該電圧を上記第3図,第4図の点
に送つた事になる。 以上のごとく、第2番目の発明と第4番目の発
明との構成は、同一の手段、回路を使用している
ことが多いが、その基本とする信号種は、上記2
つの発明では逆になつている。但し、その信号を
分極速度で割り算し、2つ以上の速度の差を検出
し、その差を記録する動作は同一である。但し、
その記録された値の単位は異なる。 次に、第1番目の発明と第2番目の発明を実施
する装置である、第3番目の発明と第4番目の発
明とを合わせた実施例について説明する。 第7図は、本発明の全体を構成した塗装金属の
塗膜下金属面の外部分極特性を、自動的に測定す
る装置のブロツク図である。該第7図の構成をな
す測定セル1から制御装置33までの内容につい
ては前述したので、以下省略するが、該実施例の
特徴は、切換スイツチ34〜39を設けたことで
ある。 該各スイツチを、図中のv側に接続することに
より、第3番目の発明、同様に該各スイツチをi
側に接続することにより、第4番目の発明のブロ
ツク図になる。すなわち、上記各スイツチをv側
にすれば、前述した第3図のブロツク図、i側に
すれば前述した第5図のブロツク図となる。従つ
て、本実施例の詳細は省略する。以上の様に、ス
イツチの切換えにより、簡単に測定方法が変更で
きる。 次に、上記装置によつて行われた実験例につい
て説明する。 〔実験例〕 実験では、塗装鋼板は「塗膜」と「鋼表面近
傍」からできており、塗装鋼板の腐食は、鋼表面
付傍に生成した局部電池の放電であるとする。そ
れ故、鋼表面近傍の分極特性は、第1に腐食状態
と関連があり、第2に塗膜が示す分極特性と塗装
鋼板が示す分極特性との差によつて表現できるも
のと想定した。 ここで、塗膜の電気的等価回路として抵抗成分
と容量成分との並列回路とすると、第14図、第
15図に示すような電流走査においてはV/k―
t関係が、電位走査においてはi/k′―t関係
が、走査速度(k:A/sec…k′:V/sec)に依
存しない曲線となる。一方、鋼表面近傍では、電
解反応の抵抗が分極の増加とともに第16図に示
したごとく変化するため、塗装鋼板のV/k―t
関係は、走査速度に依存するはずである。 塗装鋼板は、「塗膜」と「鋼表面近傍」が電気
的に直列につながつているものと仮定すれば、電
流走査法によつて種々の走査速度で測定したV/
k―t関係は、走査速度に依存しない塗膜成分と
走査速度に依存する鋼表面近傍成分が単に足し合
わされたものである。換言すれば、2つの電流走
査速度k1とk2で得たV/k1―t関係とV/k2―t
関係の差を取り出せば、塗膜に起因するV/k―
t関係は相殺されて鋼表面近傍に起因するη/k
―t関係の差のみが得られる。(ηは、鋼表面近
傍にかかる過電圧) 以上の想定のもとに、ハク離塗膜および塗装鋼
板の電流および電位走査法による分極曲線の走査
速度依存性を検討した。 実験は、鋼板(JISG3141:SPCCB)をキシレ
ン脱脂した後、ドクターブレードで塗装したもの
を塗装鋼板試料とした。ハク離塗膜は、ポリエチ
レン板、またはブリキ鋼板(GISG3303SPTE)
に塗装したものをハク離して得た。塗料は、ガラ
スフレーク含有塗料およびシアナミドヘルゴン系
常乾塗料を用いた。分極装置には、コロージヨン
レートメータ(CRM、日本ペイント(株)、AT―
101型)を用い、電流および電位を3ペン式レコ
ーダに記録した。腐食液は、3%NaCl溶液とし
た。 下記する条件により実験した。 試料: (A):合成樹脂中にガラスフレークを含有させた
塗料をブリキ鋼板に膜厚約3000μになる様
エアーレス、スプレー塗装し、自然環境で
乾燥させた後、水銀アマルガム法でブリキ
鋼板より塗膜をハク離し、ハク離塗膜とし
た。 (B):鋼板(JIS.G.3141、SPCCB)にJIS―K―
5325―1のシアナミドヘルゴン下塗赤さび
色塗料を膜厚約100μになる様エアースプ
レー塗装し、自然環境で乾燥し塗装鋼板と
した。 (C):試料Bの塗料組成の内、防錆顔料のみ含有
しない塗料を、上記試料Bと同様の方法で
塗装鋼板を作成した。 溶液:測定セル中の浸漬液(腐食液)は3%
NaCl、かつ、浸漬液の温度は40℃に保
温とした。 分極速度:定電位法にあつては、1分間に
500mV、50mV、及び10mVの速度で直
線的に増加した。一方、定電方法にあつ
ては、1秒間に3.9、8.7、17.5、及び
35.0×10-10Aの電流増加速度で直線的に
変化させた。但し、いずれも印加する方
向は、一般に還元反応を生じせしめる所
の塗膜下鋼面をより負とする方向であ
り、腐食液より塗膜を介して塗膜下鋼面
へ向う方向に電流が流れる様にした。 第1番目の実験例は、ハク離塗膜(試料A)に
ついてであり、第8図に示す測定セルを用いた。
詳しくは、電極及び溶液を入れる口を有したガラ
ス製からなる2つのガラスセルNo.1とNo.2とによ
り、ハク離塗膜を液モレの無き様、パツキングと
共にサンドイツチ状に固定し、かつ一方の室には
ハダカ鋼板W及び上記の溶液を、他方の室には基
準電極R(銀―塩化銀電極)と対極C(白金板)及
び上記の溶液を入れ、40℃に保持する一方、ハク
離塗膜と溶液との反応、(例えば、塗膜への溶液
の浸透による吸水率、並びに塗膜からの水可溶物
質の溶解率が略一定になる期間、本例では4日間
静置した。次いで、上記C―W間の電流は略ゼロ
(前述したWの自然電極電位で電解した状態)に
設定した后、上記した分極速度でWの電位を変化
させ、その時検知される電流変化と時間との関係
を測定した。その結果は、第9図に示され、前述
した2つ以上の速度で分極した時の差を検出、記
録する前の関係の図である。 第9図はハク離塗膜の分極特性として、ガラス
フレーク含有塗膜の例を示す。これは、電位走査
を行なつた場合の例である。i/k′―t関係は、
走査速度k′に依存しないとみなすことができた。
しかし、この曲線は、最初に想定した容量成分と
抵抗成分が単に並列につながつている電気的等価
回路のものとは、異なつていた。電流走査におい
ても同様であつた。 電位変化速度kx(500,50,10mV/min)で、
電流変化を割り算し、その値を分極時間(本例で
は4分間まで)との関係は、図示される様に、
kxが50倍の範囲内でも、略同じであり、今、kx
=10mV/minの分極速度を基準にして、他の2
つの速度でのi/kx―tの関係を引算し記録す
ると、第10図であり、その差は極めて小さい。
すなわち、ハク離塗膜では、本発明の方法、装置
によつて分極特性を測定することはできない。こ
の事は、前述したが、本発明の特徴とするもので
あり、例えば実際の問題として、塗装金属板に塗
膜ふくれ(ブリスター)が観察される場合等、該
塗膜ふくれを考えると、塗膜と金属との間は、溶
液が存在し、第8図のWとハク離塗膜との間に溶
液が存在することと極めて類似しており、第8図
の鋼板Wは、ガラスセルNo.1側の溶液と反応し、
腐食されやすい状態となつている。従つて、第9
図,第10図の様に、分極速度に略依存しない場
合は、塗膜の下の金属は、腐食しやすい状態で、
かつ、一般に示される塗膜異常が生じていると言
える。該検定は、図示していないが、塗装された
鋼板に塗膜ふくれが観察される試料を本実験例と
同じ様に測定しても、第10図に示される様に、
△i/kxは極めて小さく、略、分極速度に依存
しない結果が得られた事と一致する。又、上例で
は電位変化を行つてその時流れる電流変化を検知
したが、電流を印加してゆき、電位変化を検知し
ても同様な結果が得られた。 次に、第2番目の実験例は、試料B(防錆顔料
含有塗装鋼板)と、試料C(塗膜中に防錆顔料含
有無しの塗装鋼板)とを、各々定電流法により、
kx(3.9,8.7,17.5及び35.0×10-10A/sec)なる
速度で、電流を直線的に印加してゆき、その時の
電位変化を測定し、上記各々のkxで割り算し、
分極時間と相関させ、検出した。測定セルの断面
は、上記第8図と同じであり、第11図に示し
た。本実施例は、塗装された鋼板を使用したた
め、塗装鋼板裏側のセル(ガラスセルNo.1)中に
は、溶液を注入しないで実験した。塗装鋼板を試
料極Wとして基準電極R及び対極Cは、上例と同
じものを使用した。得られた結果を、第12図,
第13図に示す。第12図は塗装鋼板の分極特性
の1例を示す。これは、シアナミドヘルゴン系常
乾塗料を塗装した鋼板を35℃の設定温度で約1ケ
月間浸漬したものの電流走査における分極特性で
ある。Bは防錆顔料を含む塗料、Cは防錆顔料を
含まない塗料を塗装した鋼板のものである。第1
2図中の曲線Cは、kxを3.9〜35.0(×10-10A/
sec)に変えて測定した場合の試料Cの結果を示
したものであつて、走査速度に依存しなかつた。
一方、Bでは、明らかに走査速度依存性が認めら
れる。Cは、浸漬初期においては走査速度に依存
したが、この時点では、それは無視できるほど小
さなものとなつていた。この走査速度依存性分
は、式(1)に示すような鋼表面近傍の過電圧に関連
したものである。そして △(V/k)≡V/k1―V/k2 =η/k1―η/k2 (1) η:鋼表面近傍の過電圧 その次元は、(V/A×sec.)であり、鋼表面近
傍の抵抗変化を表わしているともいえる。鋼表面
近傍の分極抵抗が小さく、電流走査範囲で鋼表面
近傍の過電圧が数mVにしか達しない場合は、分
極抵抗は一定とみなすことができるので△(V/
k)はゼロとなる。一方、鋼表面近傍の分極が数
10mVに達する場合には、分極抵抗は、電流の関
数として変化するので△(V/k)値は、それに
かみあう値となる。図中Cが前者の場合であり、
図中Bが後者の場合であると考える。 以上のように△(V/k)値は、分極抵抗の大
小に関連するものである。ちなみに、BとCの塗
装鋼板の耐食性を比較するとBの方が良好である
ことを確認している。第13図に示す様に、kx
=35.0×10-10A/secの印加速度を基準にして、
他の速度との差を測定、記録すると、試料Cで
は、略、印加速度に依存せず、略差無しとなる。
一方、試料Bでは、印加速度に依存する。この事
は、一般に実施されている各種浸漬テストによる
肉眼観察結果を極めて良く一致する。例えば、試
料Cは、サビ、塗膜ふくれが認められ、試料Bは
極めて耐食性良好であり、サビ、塗膜ふくれが認
められない結果と本実験例の△V/kxのkxによ
る依存性と一致する。 以上の結果を考察すると、第10図に示す様
に、ハク離塗膜では分極速度に依存しないことが
明白であり、この事により本発明の意義がいつそ
う有効なものにした。すなわち、塗装された金属
を、各種の分極速度をもつて分極し、その時の差
を求めるとき、塗膜に起因するi/kx―t(第1
番目の実験例)、あるいはV/kx―t(第2番目
の実験例)関係は相殺されて、塗膜下金属面に起
因するi/kx―t、あるいはV/kx―t関係の
みの差が得られることになる。また、誤差を利用
して、塗膜下金属の腐食速度を算出することも可
能であり、更には塗料の配合(新種塗料の製造)
の検討、あるいは定量化される事から指定された
塗装金属の寿命、予測へのデータにもなりうり、
極めて、有効な評価方法、装置を提供しうるもの
であ。また、実施例に示した様に、自動的に上記
実験例を実施する装置でもあり、従来のように個
人の官能評価にたよることもなく、個人誤差も抑
制でき、更に実際の鋼構造物のモニタリングにも
活用できる装置を提供できる。なお、本発明は、
上記実験例及び実施例の装置に限定されるもので
なく、特許請求の範囲記載の要旨の範囲で種々変
更可能である。 次に、デジタル的に測定する実施例について詳
細に説明する。前述の実施例はアナログ的に測定
する方法、並びに装置についてであるが、デジタ
ル的に処理する装置について、第17図のブロツ
ク図を用いて説明する。 第17図中に記号で示したポイントは、前記
した第3図,第4図,第5図及び第6図中の記号
と同じであるが、以下、前記した第4図を用い
て説明したように電位変化を試料に印加して、そ
の時流れる電流変化を測定する装置を、第17図
では、デジタル的に測定する装置を説明する。 前記した試料に流れる電流変化は、第4図の
点では電位変化に変換されており、この変化を第
17図の第1A/D変換器101に入力し、アナ
ログよりデジタルに変換する。一方、前記した試
料に印加する電位変化率の速度kxの値を変化率
設定器102により設定し、該設定値を第2A/
D変換器103により、アナログをデジタル値に
変換する。次いで、単位時間毎に、上記第1A/
D変換器101の出力値(以下Daと称する)と、
上記第2A/D変換器103の出力値(以下kxa
と称する)とを除算するため、単位時間毎に第1
ゲート104を開き、上記2つのデジタル値を同
時に、第1演算回路105に送り込む。この第1
演算回路では、Da/kxaの演算を行わしめる機
能を有するもので、該演算が実施された直后に第
2ゲート106を開き、該演算値と同時に単位時
間を第1保持回路107に記憶する。該単位時間
は、上記電位変化率の速度kxで前記試料に電位
を印加する開始時間をゼロとし、開始と同時に前
記制御装置33からの信号で、時間制御回路10
8が作動する。この時間制御回路108は、発振
器109の発振数を読みとり、この数の積算値の
変化でもつて、時間が経過してゆく量を算定する
ものであり、上記した単位時間もこの時間制御回
路108で設定する。例えば、上記の第1ゲート
104の開閉間隔を1秒とすると、該第1ゲート
の開いている時間は、0.1秒間とし、残りの0.9秒
間は閉じておく。又、上記した第2ゲート106
の開閉間隔は、上記と同様の時間であるが、上記
第1演算回路105での演算時間はゼロでないた
め、少なくとも該演算時間分は、上記第1ゲート
104と、上記第2ゲート106との時間差とす
る。一方、上記時間制御回路108よりの信号に
より、上記第1保持回路107に上記Da/kxa
の値を単位時間毎に記憶されてゆくが、記第1保
持回路にも単位時間毎の経過時間を、単位時間毎
の上記Da/kxaの値とを対応させながら保持さ
せることが必要である。このため、上記時間制御
回路108の経過時間を第3ゲート110より単
位時間毎に、第1保持回路107に入力する。以
上の構成により、kxaなる変化率で試料の電位を
直線的に変化させてゆくときの電流変化が、上記
第1保持回路に単位時間毎に経過時間と共に保持
されてゆく。該変化を図に表わしたモデル図が第
18図であり、上記kxaを100mV/sec、単位時
間を1秒、1デジタル値を1.000×10-9アンペア
とした1測定例を示したものである。今、10秒間
通電し5秒間無通電として、10秒間の変化は表―
1に示される。上記第1保持回路107では表―
1中の単位時間と第1演算後の値とが対応して保
持されてゆく。 次いで、別なる電位変化率kxbでもつて、上記
の例での5秒后に測定したとすると、上記構成と
同様に、上記第1演算回路105で演算された
Dbなる値と、経過時間が、上記とは別の第2保
持回路111に保持されてゆく。但し、この場合
の経過時間は、上記kxbなる速度で試料に電位変
化を印加するときからの時間とすると、第18図
中の例での15秒后からの変化は表―2の様にな
り、表―2の単位時間と、第1演算后の値が、上
記と同様、第2保持回路111に保持されてい
く。 更に、次いで他の別なる電位変化率kxcでもつ
て測定すると、上記と同様、第18図の30秒間后
の変化は、表―3の単位時間と第1演算后の値と
の対応する2つづつの値が、第3保持回路112
に保持されてゆく。 以上のように、各保持回路には各々の電位変化
率でもつて測定したときの電流変化と測定時間と
が対応させながら保持されることになる。この様
に、少なくとも電位変化率kxの測定回数と保持
回路の数とは同一とすると、各々のkxでの測定
値が得られる。 次いで、前記した制御装置33の信号を用い、
各保持回路に保持された値を単位時間毎に取り出
して各電位変化率間の差を求める。今、上記実施
例に於いて、第3保持回路112に保持された値
を基準にして、上記第1、第2保持回路107,
111の値とを対比する。まず、第1保持回路1
07と第3保持回路112との値を対比する信号
を前記制御装置33より、上記時間制御回路10
8と、上記第1保持回路107及び第3保持回路
112に送り、同時に上記時間制御回路108よ
り、第4ゲート113にゲートを開く信号を送
る。以上により、第2演算回路114と、上記第
1、第3保持回路107,112とは同時に接続
されることになる。更に、該第4ゲート113を
単位時間毎に開閉させ、上記第2演算回路114
で引き算をして、各単位時間毎にその差を求め、
デジタル記録器115に、経過時間と共に記録す
る。あるいはデジタル/アナログ変換器116に
より、アナログ値に再び変換し、アナログ記録器
117に記録してもよい。上記実施例の1例が、
表―4及び表―5であり、上記表―1〜表―3の
値より求められたものである。該表―4、表―5
の1.0デジタル値は、上記した様に、この実施例
では1.000×10-9アンペアであり、上記アナログ
記録器117に記録された結果が、第19図に示
した。第19図は定電位法で測定したもので、縦
軸は電流A、横軸は電位掃引速度(V/sec)と
時間(sec)を乗じた電圧を単位として示してい
る。
The present invention relates to a method and an apparatus for measuring the polarization characteristics of a metal surface under a coating of a coated metal having a coating such as a coating. Generally, painted metal always corrodes. That is, corrosive media such as water and oxygen that have penetrated the coating film reach the metal surface beneath the coating film and undergo an electrochemical reaction. Therefore, the reaction rate and type of reaction vary depending on the type of coating film, the type of metal, the type of metal surface, the environment in which the coated metal is placed, etc. Conventionally, the method of determining the corrosion resistance of painted metal has often relied on visual inspection, and it has become a practical method of judgment based on the magnitude of rust occurrence, rust area, etc. observed on the painted metal surface. There are many. However, the development of paints with better anti-corrosion performance, better metals for coating, prediction of accidents due to corrosion, determination of when to repaint, etc. are highly desired items from an industrial perspective. In order to satisfy these requirements, relying on the conventional visual judgment method described above is extremely difficult. This is because, if we consider the point at which rust is observed on painted metal, a paint film defect occurs (for example, the paint film is destroyed), and corrosion reaction products of the metal under the paint film (red rust of iron, etc. are mainly caused by This merely indicates that iron hydroxide (iron hydroxide) is exposed to the surface of the paint film through the defect; in reality, corrosion has progressed before that point. Nevertheless, it is questionable whether it is an industrially effective method to judge rust appearing on the surface of a paint film. For example, if we consider the type of corrosion in which pores form in the metal under the paint film, it is often the case that the metal under the paint film becomes pore-formed quickly before the paint film is destroyed. This type of example can be seen especially in recent implementation methods such as thick film painting or lining. On the other hand, in addition to determining the corrosion status of the metal under the paint film, it is also important to understand the rate of deterioration of the paint film itself. For this reason, conventionally, the ion permeability of the peeling membrane,
Measurements such as water vapor permeability, oxygen permeability, dielectric loss rate, etc. are being carried out. However, these values do not necessarily correspond to the actual corrosion and anticorrosion performance of coated metals. Therefore, it is preferable to measure the properties of the coating film in its practical painted state, and these obtained (film properties mentioned above)
By linking this value with the corrosion reaction of the metal under the coating film, it seems possible to evaluate the corrosion resistance of coated steel sheets, which has industrial value. In view of the above-mentioned current situation, the inventor has made earnest efforts to
We have been working on research and development of evaluation methods. That is, the present inventors have worked on the idea of making the contents of Japanese Patent No. 960239 even more effective, for example. In other words, the above patent is 1
This method detects the relationship between the potential and current when the coated metal is polarized at one speed, excluding only the coating film resistance component. That is, in the potential-current relationship, the resistance value of the coating film is assumed to be constant. However, it has been found that there are some paint films for which it is difficult to say that the electrical resistance of all painted films remains unchanged depending on the magnitude of polarization. Based on this fact, the present invention aims to measure the polarization characteristics near the surface of the steel under the coating on a steel plate coated with a high-resistance coating, as well as to measure the polarization characteristics near the steel surface under the coating. The purpose of this study is to examine whether it is possible to evaluate the corrosion resistance of steel plates. The first feature that led to the completion of the present invention is that conventionally, the potential of the sample is increased or decreased at a certain speed in the constant potential electrolysis method.On the other hand, in the constant current method, the potential of the sample is increased or decreased at a certain speed. However, in the present invention, polarization is performed at two or more different speeds. The second characteristic is that if the polarization speed is k, then even if k is changed, the coating film alone will have v/k
The value of (v is the voltage applied to the sample...in the case of constant current electrolysis) or i/k (i is the current applied to the sample...in the case of constant potential electrolysis) does not depend on k, but it depends on painted metal. I discovered that. The third characteristic is that as a result of evaluation using conventional methods, the corrosion resistance is poor (for example, blistering occurs, rust is observed, the rust-preventive pigment is not effective, or the paint film is in poor condition at first glance). For coated metals that are determined to be normal (such as holes penetrating the metal beneath the coating film), only the coating film exhibits the second characteristic described above. In other words, even if k is changed, the value of v/k is k
does not depend on The fourth characteristic is that normally painted metal depends on k, but as painted metal deteriorates, k
By tracking this dependence, it is possible to know the deterioration rate of painted metal, which can be applied to predicting the deterioration of painted metal and monitoring painted metal. Specifically, the first invention is a method for measuring the difference in current when two or more linearly varying voltages having different speeds are applied to a coated metal, and a coated metal having a coating film and a counter electrode. is immersed in a solution, and with a non-energizing interval of one fixed time or more sufficient to return the coated metal and the opposite electrode to their original non-energized state, a completely different rate of voltage change is applied to each energizing time. Intermittently apply any of various DC voltages or currents that linearly change in a positive or negative direction, and apply any of the respective electrolytic currents or voltages that flow between the coated metal and the counter electrode during each of the energization times. Find each division value by dividing the time change per unit time by the voltage change rate of the corresponding energization time above, and use one of the division values as a reference value, and divide the reference value, other division values, and The purpose of this method is to measure the external polarization characteristics of the metal surface under the coating film of coated metal, which is characterized by extracting the difference and determining the relationship between the difference and the application time of the DC voltage. The second invention is a method of measuring the difference in potential when two or more linearly changing currents having different speeds are applied to coated metal,
The painted metal and the counter electrode are immersed in a solution, and the DC current that changes linearly in a positive or negative direction at two or more different speeds at intervals of at least 1 minute is applied to the coated metal and the opposite electrode at intervals of at least 1 minute. is applied, the time change in the potential of two or more electrodes of the coated metal is divided by each of the above speeds, and the relationship between the difference and the polarization time is measured. The purpose is to measure the external polarization characteristics of the lower metal surface. Furthermore, a third invention provides a measurement cell comprising at least a coated metal and a counter electrode immersed in a solution;
means for detecting an electrode potential difference between the coated metal and the counter electrode, means for applying and maintaining a potential substantially the same as the electrode potential difference between the coated metal and the counter electrode, and having two or more different speeds; and a means for generating a direct current potential that can be changed linearly and positive or negative and applying it between the coated metal and the counter electrode; an applying means capable of applying an electric current between the coated metal and the counter electrode; a device that measures changes in electrolytic current flowing between the coated metal and the counter electrode; dividing the two or more measured values by each of the above-mentioned speeds, and A device for storing and extracting the difference between two or more values divided by mutually corresponding times in the different positive electric times,
The present invention proposes a new device characterized by comprising a device for recording the relationship between the difference and the energization time. Further, the fourth invention provides at least a measurement cell formed by immersing a coated metal and a counter electrode in a solution;
DC current generating means having three or more different speeds and capable of changing linearly and positively or negatively; and controlling means capable of operating the DC current generating means at intervals of one minute or more. , a device for measuring the potential change of the painted metal; a device for dividing the two or more measured values by the respective speeds and storing the same; and extracting the difference between the two or more divided values; A device for measuring the difference between two or more electrolytic potentials when a coated metal is polarized at two or more different applied current speeds is provided, comprising a device for recording the relationship between the difference and the polarization time. This is what we are trying to provide. As described above, the present invention appears to be extremely similar to the conventional constant-potential electrolysis method and the device related to the method, which is a potentiostat, as well as the conventional constant-current electrolysis method and the device related to the method, which is the galvanostat. Although it is common knowledge that the present invention is characterized by changes in current and voltage when a voltage and current are applied to a sample at an arbitrary time or at a predetermined rate at regular intervals, unlike conventional methods, To measure the rate of reaction between the sample and solution (corrosion rate, etc.), change over time, etc. to make the sample a material with better corrosion resistance, or to predict the life of the sample and prevent accidents due to corrosion. It is not intended to be used when exchanging samples in advance. That is, even though the present invention has the same purpose as the conventional one,
The measured values obtained, the method used to obtain them, and the equipment used for the method are extremely novel. The first meaning of conventional methods and devices is that it is known to polarize metals at two or more different speeds, and attempts are made to determine the performance and properties of metals based on the speed dependence. is also publicly known. In other words, when the same sample or samples are polarized at different rates, the difference in polarization is the difference in reactivity between the sample and corrosion at each polarization rate, and it is clear that each sample is polarized at different rates. This is the difference between the results of different states of the sample during polarization. The second method is to obtain information on how much the sample has changed over time, including the difference between two or more polarizations at regular intervals or for a certain period of time, and is the same as the second meaning above. It is. The third method is to measure the amount of change in the sample or the content of the change, similar to the above, although a combination of the first and second methods may be implemented. However, in the present invention, the details of which will be shown in Examples described later, in the constant potential method, the obtained electrolytic current is divided by the rate of applied voltage, and two or more different applied voltage rates are used. Similarly, the electrolytic current obtained at each speed is divided by each speed, and the difference is correlated with the voltage application time to obtain information about the metal surface under the coating film. be. On the other hand, the same applies to the constant current method; in the above example, the value obtained is the electrolytic current, but in this method, the only difference is that it is the potential. That is, the present invention is to remove the value due to the coating film by dividing the current and potential obtained by polarizing the coated metal by the polarization speed, and as a result, the value near the metal surface under the coating film, The objective is to obtain information on the so-called corrosion and anticorrosion reactions of metals under coatings. Next, among the present invention, the constant potential electrolysis method, that is, the first
The basic idea of the invention will be explained using FIG. Figure 1 is related to the constant potential method.
A high input resistance converter with a counter electrode C and a high input resistance converter between the C and R.
AMPI and arithmetic unit AMP2 are interposed, and an ammeter A is connected to the above W, while a voltmeter V, an applied voltage scanning generator Vt, and a DC voltage generation/holding mechanism.
Equipped with Vo. Figure 1B shows the actual circuit configuration. In the figure, 1 is a measurement cell, which is placed in a solution such as an aqueous corrosive solution, an organic solvent, or a mixture thereof (it does not have to be a commonly used electrolyte solution). It is made by dipping the counter electrode C and the painted metal W. The counter electrode C and the coated metal W form a closed circuit via a solution, with the first DC voltage power source 2a, the second DC voltage power source 3a, the ammeter 4a, and the ON state of the switch 5a. On the other hand, the voltmeter 6a is connected to the counter electrode C and the painted metal W. 7a is a division circuit, which is connected to the ammeter 4a and the subtraction circuit 8a. On the other hand, 9a, 10
a is a memory circuit, and the former memory circuit 9a is the above C-
The latter storage circuit 10a is the division circuit 7a that stores the time change of the current flowing between C and W, and the time change of the current flowing between C and W is stored as a mark of the first DC power supply 2a. This circuit stores the value divided by the acceleration, and there is no need to temporarily store it in the former storage circuit 9a, so the basics of its operation will be described below without providing the storage circuit 9a. Now, when the switch 5a is opened and turned off, the value on the voltmeter 6a becomes the potential difference between C and W, that is, the difference between the natural electrode potentials of the counter electrode C and the painted metal W in the solution. Assuming that this is Vo, the second DC voltage power source 3a is adjusted so that the same voltage -Vo, which has a different polarity from this Vo, has the magnitude of the second DC power source 3a. Next, when the switch 5a is turned on, a potential difference -Vo, which is opposite to the potential difference Vo between C and W, is applied between C and W, so that the current in the ammeter 4a becomes approximately zero. (This state will hereinafter be referred to as the state of electrolysis at the natural electrode potential of the coated metal).
After this state is established, the first DC voltage power supply 2a described above
is operated to linearly change the voltage with an applied acceleration of k1 , and at the same time, the above-mentioned divider circuit 7a and memory circuit 10a are operated. With the above operation, C-
A current flows between W, and the time change of the current is constantly divided by k1 via the ammeter 4a, and the resulting value is stored in the memory circuit 10a as a time change. Then a predetermined time (hereinafter referred to as polarization time)
After the polarization is completed, the switch 5a is turned off, and the first and second DC voltage power supplies 2a, 3a and the divider circuit 7a are returned to their original states, and at the same time, the value obtained by the above operation is stored in the storage circuit 10a. I'll keep it. By the above operation, the painted metal has returned to its natural state (electroless state), and after keeping it in this state for more than 1 minute, the natural electrode potential of the painted metal is restored again using the second DC voltage power supply 3a as above. electrolysis, and set the value of the ammeter 4a to approximately zero. Next, the first DC power supply 2a linearly applies a DC voltage between C and W at an applied voltage speed of k2 . The electrolytic current at that time is inputted to the dividing circuit 7a via the ammeter 4a, and the value is constantly divided by k2 , and the time change of that value is stored in the memory circuit 10a, and the polarization is continued until a predetermined polarization time. do. Next, the difference between the value divided by k 1 and the value divided by k 2 is calculated by the subtraction circuit 8a while synchronizing the elapsed polarization time, and the result is measured. Alternatively, without storing the value of the time change divided by k 2 , synchronize the time change of the value divided by k 1 first with the elapsed time (polarization time) of the value divided by k 2 . Even if the subtraction circuit 8a calculates the value while doing so, the result will be the same as above. That is, even in a method in which only the first polarized value is stored and the next polarized value is not stored, the same value is obtained. Next, among the present invention, the constant current method, that is, the second
The basic idea of the invention will be explained using FIG. In Fig. 2A, 1 is a measuring cell, which is equipped with a painted metal W, a reference electrode R, and a counter electrode C. A high input resistance converter AMPI and a computing unit AMP2 are interposed between C and W. An amplifier AMP1' and a voltmeter V' are interposed between them, an ammeter A' is connected to W via a variable resistor r1 , and an applied voltage scanning generator Vx' is provided. Figure 2 (b) shows the actual circuit configuration. What is different from Figure 1 (b) is the
The DC voltage power source 2a is the DC current power source 2' in FIG.
Similarly, in FIG. 2, the second direct current power source 3a is the zero current generator 3'a, and the divider circuit 7a, memory circuit 10a, and subtraction circuit 8a each calculate and store the time change of current. The division circuit 7a, memory circuit 10a, and subtraction circuit 8 in FIG.
a is only for calculating and memorizing the potential,
For this purpose, in FIG. 2, the output of the voltmeter 6a is simply connected to the divider circuit 7a. Therefore, the basic measurement operation is the same as that shown in FIG. 1 described above. However, in Fig. 1, the second
Although the magnitude of the DC potential power supply is set to -Vo, in FIG. 2, in order to make the current between C and W zero, a zero current generator 3'a is used which applies -Io to make it zero.
With the above configuration, in Fig. 1, polarization was performed at an applied voltage rate of k 1 or k 2 , but in Fig. 2, polarization is only performed at an applied current rate of k' 1 , k' 2 , and the basic operation is as follows. Since the content is similar to that explained in FIG. 1, the explanation will be omitted. Next, the third device, which is a device for carrying out the first invention,
The embodiment of the second invention will be described in detail. As mentioned above, it is necessary that the electrode potential of the counter electrode C itself is stable in the solution and that the potential of the counter electrode C itself is stable and difficult to change even if a current flows between the counter electrode C and the coated metal W. When measuring the metal W, for example, a silver-silver chloride electrode or a calomel electrode may be used as the counter electrode C. That is, the electrical resistance of the coating film is extremely high, the electrolytic current is extremely small compared to uncoated metal, and the polarization of the counter electrode itself has little effect. However, in order to perform more accurate measurements and detect corrosion and anticorrosion reactions on metal surfaces under coatings, it is sometimes necessary to further stabilize the counter electrode itself. Therefore, in the following embodiments, at least the counter electrode C serves only as an electrode that receives current flowing in and out of the coated metal W, and in order to prevent the influence of the polarization of the counter electrode itself from being added to the measured value, The measurement cell was equipped with a reference electrode, and the signal from the reference electrode was used. That is, the first
The first invention includes a measuring means for setting in advance the error current caused by the electrode potential difference between the counter electrode C and the coated metal W to approximately zero, while the second invention includes a Equipped with a detection means that can stably measure the electrode potential difference with the painted metal W, suppressing at least the influence of the polarization of the counter electrode itself as much as possible,
The measurement signal is the polarization current of the coated metal. Next, FIG. 3 is a block diagram of an apparatus for automatically measuring the external polarization characteristics of the metal surface under the coating of coated metal according to the present invention by a constant potential electrolysis method, and FIG.
This is a wiring diagram. Hereinafter, the order of operation and each block will be explained while comparing FIG. 3 and FIG. 4. First, the measurement cell 1 includes a coated metal plate W having a film or coating made of an inorganic substance, an organic substance, or a mixture thereof on the surface, a reference electrode R exhibiting a stable electrode potential such as a calomel electrode, a silver-silver chloride electrode, and the like. Counter electrode C made of non-corrosion-resistant metal such as platinum
was immersed in a 3% NaCl corrosive solution, and the electrode potential and electrolytic current of the painted metal plate W were measured and calculated twice with an interval of 1 minute or more, and the difference was synchronized with the measurement time. The polarization characteristics of the metal surface under the coating can be measured using it. Next, the electrode potential measuring means 2 measures the resistance between the coated metal W and the reference electrode R (the electrical resistance of the coating film in the immersion liquid +
The above-mentioned standard is passed through the high input resistance converter 3 which has an input resistance sufficiently higher (usually 10 13 Ω or more) than the liquid resistance + the interfacial resistance called polarization resistance of the counter electrode surface and the metal surface under the coating film. connected to electrode R;
It is a voltmeter whose other end is grounded, and measures the electrode potential of the coated metal W while minimizing the input of the electrolytic current generated by the applied voltage described below. Specifically, the output of the converter 3 is connected to the resistor
DC amplifier AMP and resistor R 2 are grounded through R 1 and measure the potential difference across the resistor R 1 .
are connected in parallel, one end is used as the output side of the converter 3 and the other end is used as the output signal of the voltmeter, and the amplification degree can be changed by the ratio of resistors R 1 and R 2 . It's summery. Furthermore, the measurement preparation means 4 that enables electrolysis at the natural electrode potential of the painted metal W in the solution includes a servo mechanism 5 whose one end is connected to the electrode potential measurement means 2 and whose other end is grounded, and a compensation It includes a signal supply means 6, a switch 7, and a first computing device 8.
Further, to explain in detail using FIG. 4, first, the input side of the arithmetic unit 8 is connected to the high input resistance converter 3
and potentiometer P 1 of the compensation signal supply means 6
and the output side of the means is grounded via the closed state of the switch 7 (connection between c and d). The output side of the calculator 8 is connected to the counter electrode c, and calculates the output (electrode potential signal) a of the high input resistance converter 3 and the output (compensation potential signal) b of the compensation signal supply means 6. , the above painted metal W
The error current caused by the electrode potential difference between the electrode C and the counter electrode C is made approximately zero. Further, the servo mechanism 5 includes a comparator 9, a servo motor 10, and a comparison signal supply means 11, forming a negative feedback circuit. Specifically, the input side of the comparator 9 is the DC amplifier of the electrode potential measuring means 2 described above.
It is connected to the output of the AMP and also to the comparison signal supply means 11, while the output side is a normally open contact L 1
The output (potential signal) Va of the electrode potential measuring means 2 and the output (comparison signal) of the comparison signal supply means 11 are connected to the servo motor 10 via
The output, which is the signal of the difference, is compared with Va.
By turning on (closed) the normally open contact L1 , an input signal is input to the servo motor 10 to drive the motor. The potentiometer P1 of the above-mentioned compensation signal supply means 6 and the potentiometer P2 of the above-mentioned comparison signal supply means 11 are linked to the drive of the servo motor 10 . The supply means 6 is a potentiometer P1
, a DC power supply E 1 , and distribution resistors R 3 and R 4 are connected in parallel, and the switch 7 is connected in the closed state (c-
The output voltage (compensation signal) a of the means 6 is connected to the first arithmetic unit 8 through the potentiometer P1.
is input to the first arithmetic unit 8 while being constantly compensated for by the drive of the servo motor 10. On the other hand, the potentiometer P 2 of the comparison signal supply means 11 is connected to the DC power supply E 2 and the distribution resistor R 5 ,
R 6 is connected in parallel with the distribution resistor R 5 ,
The branch point of R6 is grounded, and the potentiometer P2 is connected to the above-mentioned comparator 9 to input the comparator signal -Va. Then, normally open contact L 1 is turned on (closed)
By doing so, the inputs Va and -Va of the comparator 9 are compared, and the servo motor 10 is driven so that the above-mentioned potentiometer P2 is displaced so that the difference becomes approximately zero, and at the same time the above-mentioned The potentiometer P1 of the compensation signal supply means 6 is also displaced, and the potential difference between a and b of the first arithmetic unit 8 becomes approximately zero, and as a result, the servo motor 10 is stopped. With the above configuration, preparation for measurement is performed, and the output of the first computing unit 8 described above becomes approximately zero, and as a result, the electrolytic current between the counter electrode c and the coated metal W described above becomes approximately zero. This preparation state is the state in which the coated metal W is electrolyzed at its natural electrode potential. Hereinafter, this state will be referred to as the first preparation state. Next, a power supply 12 that applies a DC voltage having a positive or negative linear gradient to the painted metal W is constructed by connecting a potentiometer P 3 , a DC power supply E, and distribution resistors R 7 and R 8 in parallel. Therefore, the output example of potentiometer P3 is the open contact side e of the switch 7 mentioned above,
It is connected to the branch point of the distribution resistors R 3 and R 4 of the compensation signal supply means 6 via the common contact c, and the branch point of the distribution resistors R 7 and R 8 is grounded. . With the above configuration, a DC voltage with a positive or negative slope is outputted from the DC voltage application power supply 12 by the displacement of the potentiometer P3 , and if the switch 7 described above is connected between ce and e, the above compensation is achieved. Superimposed on the output voltage of the signal supply means 6,
It can be input to the input b side of the first computing unit 8, and as a result, the superimposed voltage is applied to the counter electrode c via the computing unit. The device 13 for measuring the electrolytic current flowing through the branches of the coated metal then comprises a DC amplifier 14 and a multi-stage resistor 15. For details, see DC amplifier 1.
4 is connected in parallel with resistor R 9 , and its input side is connected to the painted metal W and is grounded via multistage resistor 15 . That is,
The multistage resistor 15 is a normally closed contact with the resistors R10 to R13 .
L 2 and the normally open contacts L 3 to L 5 are each connected in series and the whole is connected in parallel so that an appropriate voltage drop can be obtained by switching the contacts, and the resistors R 10 to The degree of amplification of the output voltage of the DC amplifier 14 can be changed by changing the resistance value of R 13 and the resistance value of the resistor R 9 described above. Therefore, the electrolytic current flowing between the counter electrode c and the coated metal W is converted into voltage and detected. Next, after the above-described first preparation state, the output of the DC voltage applying power source 12 can generate a DC voltage at a speed having a positive or negative linear slope, so that the potentiometer P 3 is adapted to be displaced at a constant speed by a synchronous motor 16, and this displacement speed kx (V/sec) is controlled by a displacement control means 17. As described above, if the synchronous motor 16 is driven to apply a DC potential (V/sec=kx) with a positive or negative potential gradient to the painted metal W using the counter electrode c, the corresponding painted metal The electrolytic current change of W receives an appropriate voltage drop by the multi-stage resistor 15 of the electrolytic current measuring device 13, is input to the DC amplifier 14, is amplified, and is then output as a measurement signal.
The output voltage is input to the dividing circuit 18 and divided by the displacement speed kx of the DC voltage applying power source 12 described above. Specifically, the division circuit 18 is connected to the DC amplifier 1
9. Equipped with a multi-stage resistor 20 and a DC amplifier 1
9 is connected in parallel with the resistor R 14 , and its input side is connected to the electrolytic current measuring device 13 and grounded via the multistage resistor 20 . Further, the output side is connected to a switch 21.
The multistage resistor 20 is a normally closed contact with resistors R 15 to R 18
L 6 and the normally open contacts L 7 to L 9 are each connected in series, and the whole is connected in parallel so that an appropriate voltage drop can be obtained by switching the contacts, and the resistor R 15 The change in the electrolytic current described above is divided by the displacement speed kx using the resistance value of ~ R18 and the resistance value of the resistor R14 . That is, the time change i-t of the electrolytic current i is always divided by kx, and that value is always used as the output of the DC amplifier 19. This can be obtained by setting a suitable resistance value. Next, the time change of the value output by the division circuit 18 is determined by the switch 21 (connected between f and g),
and is stored in the first storage circuit 22 through the closed state of the normally open contact L10 . Specifically, when a direct current voltage is linearly applied positively or negatively to the coated metal W by the counter electrode C at the speed kx, the coated metal W
The time change of the electrolytic current flowing through the circuit is divided by the value kx, and the resulting time change is stored in the first memory circuit 2.
2. When the polarization is completed for a predetermined period of time, the normally open contact L10 is opened to stop the memorization and end the measurement. Then, a signal is sent from the control device 33 via the dotted line shown in FIG. 3 to wait for one minute or more until the next measurement and to return each means circuit switch to its original state. For example, the switch 7 is switched to the connection between c and d, and the output voltage of the DC voltage applying power source 12 is set to zero.
The potentiometer P3 is returned to the starting state via the synchronous motor 16. With the above configuration, from the first preparation state described above, the coated metal W can be polarized with the applied velocity kx, and the electrolytic current it at that time is divided by k.
The value of t/k is now stored in the storage circuit.
This is hereinafter referred to as the first measurement. Note that the first storage circuit 22 is a storage type synchroscope,
Alternatively, there are many methods, such as connecting many ordinary hold-type digital voltmeters in parallel.
Details are omitted. Next, after the first measurement is completed, the same operations and configuration as described above up to the first preparation state are repeated for one minute or more, and the potentiometers P 1 and P 2 are automatically controlled by the servo motor 10. adjusted to
The electrolytic current flowing between the counter electrode C and the coated metal W is always approximately zero. In other words, it is in a state where it is electrolyzed at the natural electrode potential of the coated metal. Hereinafter, this will be referred to as the second preparation state. Next, after waiting for more than one minute, the switch is connected between ce and e as described above, and the synchronous motor 16 is driven at the speed k'x,
While displacing the potentiometer P3 at a speed of kx, the normally closed contact of the multistage resistor 20
L 6 is open, normally open contact L 7 is closed, and resistor R 16 is grounded. Further, the switch 21 is switched to the connection between f and h, and the switch 24 is connected between j and l, the normally open contact L11 is closed, and the first memory circuit is connected to a similar second memory circuit. 23, the value obtained by dividing the time change (i'-t) of the electrolytic current by the applied acceleration (k'x) is always stored in the same way as described above. The state measured with this configuration is hereinafter referred to as the second measurement. However, the second measurement is particularly different from the first measurement described above because the displacement control means 17
The displacement speed of the potentiometer P3 , which is controlled by , has become k'x. When the painted metal W is polarized for a predetermined time, the normally open contact L11 is opened to stop the memory in the second memory circuit 23, and the switch 7 is connected between c and d. the potentiometer so that the output voltage of the DC voltage applying power source 12 becomes zero.
P3 is returned to the starting state by the synchronous motor 16 mentioned above. With the above configuration, the memory circuits 22 and 23 store potential changes over time (originally, this time change is a value obtained by dividing the time change in the current flowing through the painted metal W by a predetermined value, but as described above, In this embodiment, the electrolytic current measuring device 13 is configured to convert DC current into DC voltage and output it.)
is stored. For more information, please visit it/
kx and i'-t/k'x are stored. Next, the first memory circuit 22 and the second memory circuit 23 connect to the difference detector 2 via the normally open contacts L 12 and L 13 .
4 and are respectively connected to the recording device 25. Specifically, the difference detector 24 includes a second computing unit 26 and a voltmeter 2.
7, and the input of the second arithmetic unit 26 is
The first memory circuit 22 via the normally open contact L12 .
and the second memory circuit 23 via the normally open contact L13 , and the output thereof is grounded via a voltmeter 27. On the other hand, the output of the voltmeter is connected to the recording device 25, such as an ordinary pen recorder, oscilloscope, synchroscope, or the like. Next, the normally open contacts L 12 and L 13 are closed, and the first memory circuit 22 and the second memory circuit 2 are closed.
3 are operated simultaneously and are input to the second computing unit 26 while being temporally synchronized, the difference between m and q of the computing unit 26, specifically, the first
i-t/kx stored in the memory circuit 22 and i′- stored in the second memory circuit 23 mentioned above.
If the difference (△i/k) from t/k'x is detected by the second arithmetic unit 26 and its output is recorded in the recording device 25 via the voltmeter 27, then
The desired external polarization characteristics of the metal surface under the coating film of the coated metal can be obtained. On the other hand, the switch 28 is connected between j and n to close the normally open contact L 14 , and at the same time the above-mentioned second measurement is started, the i-t/kx stored in the above-mentioned first memory circuit is , by sequentially closing the normally open contact L 12 and sending it to the second computing unit 26,
The above △i/k is the same as above, the recording device 25
will be recorded in the second storage circuit 22.
becomes unnecessary. However, two or more of the above displacement speeds
Measure kx and calculate the difference △ at each value of kx
It cannot be said that it is suitable for detecting and recording i/kx.
This can be achieved by repeatedly using the first memory circuit 22 and the second memory circuit 23. For example, k 1 in the first measurement, k 2 in the second measurement, and k 2 in the third measurement.
k 3 and k 4 in the fourth measurement, the values at k 1 and k 2 are stored in the first storage circuit and the value at k 2 in the second storage circuit, respectively, and it/t/ at k 3 at the third measurement is stored. k 3 is stored in the first storage circuit. While removing the value of i-t/k 1 , or before the third measurement, i-t/k 1
The value of is set to zero and stored in the first storage circuit. Then, the difference between it/k 3 in the first storage circuit and it/k 2 in the second storage circuit is recorded by a recording device. Then, similarly, the object of the present invention can be achieved by sequentially switching the values obtained with k 2 to zero and storing the value of k 4 . Alternatively, as many memory circuits as the number of kx required may be provided. FIG. 3 also shows a control device 33 that controls each of the above-mentioned devices, circuits, contacts, and switches, performs synchronous operation of the memory circuits 22 and 23, starts, stops, and speed controls the synchronous motor, etc. At least the connection of the control signal of the control device 33 is shown by dotted lines, but since the basics of its operation have been described above, the following description will be omitted. Next, an embodiment of the fourth invention, which is an apparatus for implementing the second invention, will be described in detail. FIG. 5 is a block diagram of an apparatus according to the present invention for automatically measuring external electrode characteristics of a metal surface under a coating film of a coated metal by a constant current electrolysis method, and FIG. 6 is a wiring diagram thereof. While comparing Figures 5 and 6, as well as the aforementioned Figures 3 and 4,
The operation order and each block will be explained. First, the measurement cell 1 and the provision of a solution, a counter electrode C, a coated metal W, and a reference electrode R in the measurement cell 1 have been described above (the embodiment has already been explained using FIGS. 3 and 4). Similarly, a high input resistance converter 3, a switch 7, a first computing unit 8, a DC voltage applying power source 1
2. The synchronous motor 16 and the displacement control means 17 are the same as those shown in FIGS. 3 and 4, so details of individual operations and blocks will be omitted. th and 4th
Only the portion related to the second invention will be explained in detail. The painted metal W is grounded via a current control variable resistor 29 and directly connected to the high input resistance converter 3, and the output of the high input resistance converter 3 is connected to the input of the first computing unit 8. a, and the output of the first arithmetic unit 8 is connected to the counter electrode C. On the other hand, the input b of the first arithmetic unit is c-d of the switch 7.
grounded through a connection between the That is, the inputs a and b of the first arithmetic unit 8 are closed by the current control variable resistor through the ground, and the output of the first arithmetic unit 8 becomes zero. Therefore, no current flows between the counter electrode C and the coated metal W, and electrolysis occurs at the natural electrode potential of the coated metal W described above. Next, the above switch is connected between ce and the potentiometer of the DC voltage applying power source 12 mentioned above.
When P 3 is driven at the speed of the synchronous motor 16 using the displacement control means 17, the output voltage of the DC voltage applying power source 12 is applied between the counter electrode C and the coated metal W. However, since the above-mentioned current control variable resistor 29 is connected between the painted metal W and the ground, voltage application control between the counter electrode C and the painted metal W is not performed, and the voltage applied between the counter electrode C and the painted metal W is not controlled. The current application is controlled between That is, the speed at which a linear current is applied between the counter electrode and the painted metal W is k'i (A/sec), and the linear potential change rate of the output voltage of the DC voltage applying power source 12 is k'v (mv/mv/sec). min), electrical resistance value r' (Ω) of the variable resistor 29 for current control.
Then, k′i is expressed by the following equation. k′i=k′v/r′×60×1000 (A/sec) Therefore, by changing the driving speed of the potentiometer P3 and the value of the current control variable resistor 29, the above A positive or negative linear current change can be given between the counter electrode C and the painted metal W, and therefore, in order to give the above-mentioned positive or negative linear voltage change between the counter electrode C and the painted metal W, the above-mentioned DC voltage application power supply 12 and synchronous motor 1
6 displacement control means 17 was used, but it can be said that it is extremely convenient because the same means can be used. Next, a voltmeter 30 is installed between the reference electrode R and the painted metal W in order to track the change in electrode potential of the painted metal W when a linear current change is applied between the counter electrode C and the painted metal W. It is being Specifically, the reference electrode R is connected to the input of the DC amplifier 32 via a high input resistance converter 31 having an input resistance sufficiently higher (usually 10 13 Ω or more) than the resistance between the painted metal W and the reference electrode R. connected to S, one of the sides, and
The t side, which is one of the other inputs of the DC amplifier 32, is connected to the painted metal W. With the above configuration, when a current is applied between the counter electrode C and the painted metal W, the potential change between the reference electrode R and the painted metal W can be detected as the output of the DC amplifier. can. Next, the output y of the voltmeter 30 is now a point in FIG. 6, which corresponds to a point in FIG. 5, and the output y is connected to the input of the above-mentioned divider circuit 18. The switch 21, the first memory circuit 22, the second memory circuit 23, and the difference detector 2 shown in FIG.
4. The configuration, connection, and operation details of each recording device are the same as those explained using FIGS. 3 and 4 above. That is, the points in FIGS. 5 and 6 are the same as the points in FIGS. 3 and 4. The content of the explanation of the embodiment using FIGS. 3 and 4 is that "a voltage is applied to the painted metal W, the current is detected as a response signal, and the current is converted to a voltage", and the voltage is It is used to detect and record the division and the difference between the two signals.
The content of the explanation of the embodiment using FIGS. 3 and 6 is that "a current is applied to the painted metal W, a voltage is detected as a response signal," and the voltage is sent to the points shown in FIGS. 3 and 4 above. It's going to happen. As mentioned above, the configurations of the second invention and the fourth invention often use the same means and circuits, but the basic signal types are different from those of the second invention.
In one invention, the opposite is true. However, the operations of dividing the signal by the polarization speed, detecting the difference between two or more speeds, and recording the difference are the same. however,
The units of the recorded values are different. Next, an embodiment that combines the third invention and the fourth invention, which is an apparatus for carrying out the first invention and the second invention, will be described. FIG. 7 is a block diagram of an apparatus for automatically measuring the external polarization characteristics of a metal surface under a coating of a coated metal, which constitutes the entirety of the present invention. Since the contents of the measuring cell 1 to the control device 33 having the configuration shown in FIG. 7 have been described above, the details will be omitted below, but the feature of this embodiment is that changeover switches 34 to 39 are provided. By connecting each switch to the v side in the figure, the third invention similarly connects each switch to i.
By connecting to the side, it becomes a block diagram of the fourth invention. That is, if each of the above switches is set to the v side, the block diagram shown in FIG. 3 is obtained, and if it is set to the i side, the block diagram shown in FIG. 5 is obtained. Therefore, details of this embodiment will be omitted. As described above, the measurement method can be easily changed by switching the switch. Next, an example of an experiment conducted using the above device will be explained. [Experiment example] In the experiment, a painted steel plate is made up of a ``paint film'' and a ``near the steel surface,'' and the corrosion of the painted steel plate is assumed to be the discharge of a local battery generated near the steel surface. Therefore, it was assumed that the polarization characteristics near the steel surface are firstly related to the corrosion state, and secondly can be expressed by the difference between the polarization characteristics exhibited by the coating film and the polarization characteristics exhibited by the coated steel plate. Here, if the electrical equivalent circuit of the coating film is a parallel circuit of a resistance component and a capacitance component, then in current scanning as shown in FIGS. 14 and 15, V/k-
In potential scanning, the t relationship and the i/k'-t relationship are curves that do not depend on the scanning speed (k: A/sec...k': V/sec). On the other hand, near the steel surface, the resistance of the electrolytic reaction changes as the polarization increases, as shown in Figure 16.
The relationship should depend on the scanning speed. Assuming that the "paint film" and "near the steel surface" are electrically connected in series, the coated steel sheet has a V/V measured at various scanning speeds using the current scanning method.
The kt relationship is simply the sum of the coating film component that does not depend on the scanning speed and the component near the steel surface that depends on the scanning speed. In other words, the V/k 1 -t relationship obtained at two current scanning speeds k 1 and k 2 and the V/k 2 -t
If we take out the difference in the relationship, V/k due to the coating film
The t relationship is canceled out and η/k due to the vicinity of the steel surface
- Only the difference in the t relationship is obtained. (η is the overvoltage applied near the steel surface) Based on the above assumptions, the scanning speed dependence of the polarization curve of the peeling coating film and the coated steel plate using the current and potential scanning method was investigated. In the experiment, a steel plate (JISG3141: SPCCB) was degreased with xylene and then painted with a doctor blade as a coated steel plate sample. The release coating is made of polyethylene plate or tin steel plate (GISG3303SPTE)
It was obtained by peeling off the painted material. As the paint, a glass flake-containing paint and a cyanamide hergon-based air-drying paint were used. The polarization device includes a corrosion rate meter (CRM, Nippon Paint Co., Ltd., AT-
101 model), and the current and potential were recorded on a three-pen recorder. The etchant was a 3% NaCl solution. The experiment was conducted under the conditions described below. Sample: (A): A paint containing glass flakes in a synthetic resin was applied to a tin plated steel plate by airless spray painting to a film thickness of approximately 3000μ, dried in a natural environment, and then painted on the tin plated steel plate using the mercury amalgam method. The film was peeled off to obtain a peel-off coating. (B): JIS-K- on steel plate (JIS.G.3141, SPCCB)
5325-1 cyanamide hergon undercoat red rust color paint was air sprayed to a film thickness of approximately 100μ, dried in a natural environment, and made into a coated steel plate. (C): A coated steel plate was prepared in the same manner as Sample B using a paint composition of Sample B that did not contain any antirust pigments. Solution: Immersion liquid (corrosion liquid) in the measurement cell is 3%
The temperature of NaCl and the immersion liquid was kept at 40°C. Polarization rate: per minute for constant potential method
It increased linearly at rates of 500mV, 50mV, and 10mV. On the other hand, in the constant voltage method, 3.9, 8.7, 17.5, and
The current was varied linearly at a rate of increase of 35.0×10 -10 A. However, the direction in which the current is applied is generally the direction that makes the steel surface under the coating where the reduction reaction occurs more negative, and the current is applied in the direction from the corrosive liquid to the steel surface under the coating through the coating. I let it flow. The first experimental example was about a peel release coating (sample A), and the measurement cell shown in FIG. 8 was used.
Specifically, two glass cells No. 1 and No. 2 made of glass each having an electrode and an opening for introducing a solution fix the peeling coating film in a sandwich shape with packing so that there is no liquid leakage, and The naked steel plate W and the above solution were placed in one chamber, and the reference electrode R (silver-silver chloride electrode), counter electrode C (platinum plate) and the above solution were placed in the other chamber, and the temperature was maintained at 40°C. The reaction between the release coating film and the solution (for example, the period during which the water absorption rate due to penetration of the solution into the coating film and the dissolution rate of water-soluble substances from the coating film are approximately constant; in this example, it is left to stand for 4 days) Next, after setting the current between C and W to approximately zero (a state in which W is electrolyzed at its natural electrode potential as described above), the potential of W is changed at the polarization rate described above, and the current change detected at that time is The relationship between and time was measured. The results are shown in Figure 9, which is a diagram of the relationship before detecting and recording the difference when polarizing at two or more speeds as described above. An example of a coating film containing glass flakes is shown as the polarization characteristics of a peel-release coating film.This is an example when potential scanning is performed.The i/k'-t relationship is
It could be considered that it does not depend on the scanning speed k'.
However, this curve was different from the electrical equivalent circuit that was initially assumed, in which the capacitance and resistance components were simply connected in parallel. The same was true for current scanning. At potential change rate kx (500, 50, 10mV/min),
The relationship between dividing the current change and the polarization time (up to 4 minutes in this example) is as shown in the figure.
Even if kx is within the range of 50 times, it is almost the same, and now kx
= 10 mV/min polarization rate as the reference, and the other 2
When the i/kx-t relationship at the two speeds is subtracted and recorded, it is shown in FIG. 10, and the difference is extremely small.
That is, the polarization characteristics of peel-release coatings cannot be measured by the method and apparatus of the present invention. As mentioned above, this is a feature of the present invention. For example, when paint film blisters are observed on a painted metal plate as a practical problem, considering the paint film blisters, A solution exists between the film and the metal, which is very similar to the presence of a solution between W and the peeling film in Fig. 8, and the steel plate W in Fig. 8 has glass cell No. .Reacts with the solution on the 1st side,
It is susceptible to corrosion. Therefore, the ninth
As shown in Fig. 10, if the polarization rate is not substantially dependent, the metal under the coating is in a state where it is easy to corrode.
Moreover, it can be said that the commonly observed coating film abnormality has occurred. Although this test is not shown, even if a sample in which paint film blistering is observed on a painted steel plate is measured in the same manner as in this experimental example, as shown in Fig. 10,
Δi/kx is extremely small, which is consistent with the fact that the result is almost independent of the polarization rate. Further, in the above example, the potential was changed and the current change flowing at that time was detected, but the same result could be obtained by applying a current and detecting the potential change. Next, in the second experimental example, sample B (painted steel sheet containing anti-rust pigment) and sample C (painted steel sheet without anti-rust pigment in the coating film) were each tested using the constant current method.
Apply current linearly at a rate of kx (3.9, 8.7, 17.5 and 35.0×10 -10 A/sec), measure the potential change at that time, and divide by each of the above kx,
It was detected by correlating it with the polarization time. The cross section of the measurement cell is the same as that shown in FIG. 8 above, and is shown in FIG. 11. In this example, since a painted steel plate was used, the experiment was conducted without injecting a solution into the cell (glass cell No. 1) on the back side of the painted steel plate. A painted steel plate was used as the sample electrode W, and the reference electrode R and counter electrode C were the same as in the above example. The obtained results are shown in Figure 12,
It is shown in FIG. FIG. 12 shows an example of polarization characteristics of a painted steel plate. This is the polarization characteristic in current scanning of a steel plate coated with cyanamide hergon-based air-drying paint that was immersed for about a month at a set temperature of 35°C. B is a steel plate coated with a paint containing a rust preventive pigment, and C is a steel plate coated with a paint that does not contain a rust preventive pigment. 1st
Curve C in Figure 2 shows kx of 3.9 to 35.0 (×10 -10 A/
sec), and the results were not dependent on the scanning speed.
On the other hand, in B, scanning speed dependence is clearly observed. Although C depended on the scanning speed at the initial stage of immersion, it had become negligibly small at this point. This scanning speed dependency is related to the overvoltage near the steel surface as shown in equation (1). And △(V/k)≡V/k 1 - V/k 2 = η/k 1 - η/k 2 (1) η: Overvoltage near the steel surface Its dimension is (V/A x sec.) This can be said to represent the resistance change near the steel surface. If the polarization resistance near the steel surface is small and the overvoltage near the steel surface reaches only a few mV in the current scanning range, the polarization resistance can be regarded as constant, so △(V/
k) becomes zero. On the other hand, the polarization near the steel surface is
When reaching 10 mV, the polarization resistance changes as a function of the current, so the Δ(V/k) value becomes a value that meshes with it. C in the figure is the former case,
B in the figure is considered to be the latter case. As described above, the Δ(V/k) value is related to the magnitude of polarization resistance. Incidentally, when comparing the corrosion resistance of coated steel plates B and C, it has been confirmed that B is better. As shown in Figure 13, kx
=35.0×10 -10 Based on the applied acceleration of A/sec,
When the difference from other speeds is measured and recorded, sample C is almost independent of the applied acceleration and shows almost no difference.
On the other hand, sample B depends on the applied acceleration. This fact agrees extremely well with the results of visual observation from various commonly performed immersion tests. For example, sample C has rust and paint blistering, while sample B has extremely good corrosion resistance, with no rust or paint blistering, which is consistent with the dependence of △V/kx on kx in this experimental example. do. Considering the above results, as shown in FIG. 10, it is clear that the release coating film does not depend on the polarization rate, and this makes the meaning of the present invention even more effective. In other words, when a coated metal is polarized with various polarization speeds and the difference is determined, the i/kx-t (first
(2nd experimental example) or V/kx-t (2nd experimental example) relationship is canceled out, and the difference only in the i/kx-t or V/kx-t relationship due to the metal surface under the coating is canceled out. will be obtained. In addition, it is also possible to use the error to calculate the corrosion rate of metal under the paint film, and even calculate the composition of paint (manufacturing new types of paint).
It can also be used as data for predicting the lifespan of a specified painted metal by examining or quantifying it.
This provides an extremely effective evaluation method and device. In addition, as shown in the examples, it is also a device that automatically performs the above experimental examples, and does not rely on individual sensory evaluations as in the past, suppressing individual errors. We can provide equipment that can also be used for monitoring. In addition, the present invention
The present invention is not limited to the apparatuses of the above experimental examples and examples, and various modifications can be made within the scope of the claims. Next, an example of digital measurement will be described in detail. Although the above-mentioned embodiments are about the analog measuring method and apparatus, the digital processing apparatus will be explained using the block diagram of FIG. 17. The points indicated by symbols in Fig. 17 are the same as the symbols in Figs. 3, 4, 5, and 6 described above, but below, the points indicated by symbols are explained using Fig. 4 described above. An apparatus for applying a potential change to a sample and measuring a change in the current flowing at that time, as shown in FIG. 17, will be described. FIG. The change in the current flowing through the sample described above is converted into a potential change at the point in FIG. 4, and this change is input to the first A/D converter 101 in FIG. 17, where it is converted from analog to digital. On the other hand, the value of the speed kx of the potential change rate applied to the sample described above is set by the change rate setting device 102, and the set value is set in the second A/
A D converter 103 converts analog to digital values. Next, for each unit time, the above 1A/
The output value of the D converter 101 (hereinafter referred to as Da),
The output value of the second A/D converter 103 (hereinafter kxa
), the first
The gate 104 is opened and the two digital values are simultaneously sent to the first arithmetic circuit 105. This first
The arithmetic circuit has a function of calculating Da/kxa, opens the second gate 106 immediately after the calculation is performed, and simultaneously stores the calculated value and the unit time in the first holding circuit 107. . The unit time is defined as zero, the start time of applying a potential to the sample at the rate kx of the potential change rate, and at the same time as the start time, a signal from the control device 33 is applied to the time control circuit 10.
8 is activated. This time control circuit 108 reads the number of oscillations of the oscillator 109 and calculates the amount of time elapsed due to changes in the integrated value of this number.The above-mentioned unit time is also determined by this time control circuit 108. Set. For example, if the opening/closing interval of the first gate 104 is 1 second, the first gate is open for 0.1 seconds and remains closed for the remaining 0.9 seconds. In addition, the second gate 106 described above
The opening/closing interval is the same time as above, but since the calculation time in the first calculation circuit 105 is not zero, at least the calculation time is the same as that between the first gate 104 and the second gate 106. Time difference. On the other hand, a signal from the time control circuit 108 causes the first holding circuit 107 to output the Da/kxa.
The value of is stored for each unit time, but it is necessary to also store the elapsed time for each unit time in the first holding circuit while correlating it with the value of Da/kxa for each unit time. . Therefore, the elapsed time of the time control circuit 108 is input from the third gate 110 to the first holding circuit 107 every unit time. With the above configuration, the current change when the potential of the sample is linearly changed at a rate of change of kxa is held in the first holding circuit with the elapsed time every unit time. Figure 18 is a model diagram that graphically represents this change, and shows one measurement example where the above kxa is 100 mV/sec, the unit time is 1 second, and 1 digital value is 1.000 × 10 -9 ampere. . Now, when the current is applied for 10 seconds and the electricity is not applied for 5 seconds, the changes over the 10 seconds are shown in the table below.
1. In the first holding circuit 107, the table -
The unit time in 1 and the value after the first calculation are held in correspondence. Next, if a different potential change rate kxb is measured after 5 seconds in the above example, the first arithmetic circuit 105 calculates the
The value Db and the elapsed time are held in a second holding circuit 111 different from the one described above. However, if the elapsed time in this case is the time from when the potential change is applied to the sample at the rate kxb above, then the change after 15 seconds in the example in Figure 18 will be as shown in Table 2. , the unit time in Table 2 and the value after the first operation are held in the second holding circuit 111 in the same way as above. Furthermore, when measuring at another potential change rate kxc, the change after 30 seconds in Figure 18 is the same as above, and the change after 30 seconds in Table 3 corresponds to the unit time and the value after the first calculation. The value of the third holding circuit 112 is
will be retained. As described above, each holding circuit holds the current change measured at each potential change rate and the measurement time in correspondence with each other. In this way, if at least the number of times the potential change rate kx is measured and the number of holding circuits are the same, a measured value at each kx can be obtained. Next, using the signal from the control device 33 described above,
The values held in each holding circuit are taken out every unit time and the difference between each potential change rate is determined. Now, in the above embodiment, based on the value held in the third holding circuit 112, the first holding circuit 107, the second holding circuit 107,
111. First, the first holding circuit 1
A signal comparing the values of 07 and the third holding circuit 112 is sent from the control device 33 to the time control circuit 10.
8 to the first holding circuit 107 and the third holding circuit 112, and at the same time, the time control circuit 108 sends a signal to open the fourth gate 113. As a result of the above, the second arithmetic circuit 114 and the first and third holding circuits 107 and 112 are connected at the same time. Furthermore, the fourth gate 113 is opened and closed every unit time, and the second arithmetic circuit 114
Subtract with and find the difference for each unit time,
It is recorded on the digital recorder 115 along with the elapsed time. Alternatively, it may be converted back into an analog value by the digital/analog converter 116 and recorded in the analog recorder 117. One example of the above embodiment is
Tables 4 and 5 are obtained from the values in Tables 1 to 3 above. Table-4, Table-5
As mentioned above, the 1.0 digital value of is 1.000×10 -9 ampere in this embodiment, and the result recorded in the analog recorder 117 is shown in FIG. FIG. 19 shows measurements made using a constant potential method, with the vertical axis representing current A and the horizontal axis representing voltage obtained by multiplying potential sweep rate (V/sec) by time (sec).

【表】【table】

【表】【table】

【表】【table】

【表】【table】

【表】【table】

【表】 上記実施例に詳記した如く、本発明にかゝる塗
装金属における塗膜下金属面の外部分極特性の測
定方法は、塗膜を有する塗装金属と対極とを測定
セルの溶液中に浸漬し、夫々異なる電圧又は電流
の変化率で直線的に変化する少くとも3種以上の
直流電圧又は電流を各々の間に一定の非通電間隔
をおいて上記塗装金属と対極間に次々と断続的に
印加して、該印加直流電圧又は電流によつて上記
塗装金属と対極間に生じる電解電流又は電解電圧
の変化を測定し、かつ該測定値を上記各印加時間
毎に夫々対応する該当の上記変化率で除算しての
ち、特定の変化率における該除算値と少くとも2
種以上の他の変化率における夫々の除算値とを互
に減算して得た少くとも2種以上の減算値を夫々
の上記印加時間と対応した関係で相互に比較させ
るようにしたことを特徴とするものであり、また
塗装金属における塗膜下金属面の外部分極特性の
測定方法を実施する装置は、塗膜を有する塗装金
属と対極とを溶液中に浸漬してなる測定セルと、
上記塗装金属と対極との間の電位差をなくする手
段と、少くとも3種以上の異なる電圧又は電流の
変化率で直線的に変化する直流電流又は電流を発
生する手段と、該発生手段で発生した夫々異なる
電圧又は電流の変化率で直線的に変化する少くと
も3種以上の直流電圧又は電流を各々の間に一定
の非通電間隔をおいて上記塗装金属と対極間に
次々と断続的に印加する手段と、該印加手段で印
加した直流電圧又は電流によつて上記塗装金属と
対極間に生じる電解電流又は電解電圧の変化を測
定する手段と、かつ少なくとも該測定手段の測定
値を上記各印加時間毎に夫々対応する該当の上記
変化率で除算する回路、該除算回路の除算値で、
特定の変化率における該除算値と少くとも2種以
上の他の変化率における夫々の除算値の間の差を
減算する回路及び該減算回路で得た少くとも2種
以上の減算値を夫々の上記印加時間と対応させた
関係で記憶する回路を持つ上記測定手段の測定値
の演算手段とを備えて成るものであり、したがつ
て上記の如き単純な方法及び簡単な構造で塗装金
属における塗膜下金属面の外部分極特性を容易か
つ確実に測定することが出来る利点を有するもの
である。
[Table] As detailed in the above example, the method for measuring the external polarization characteristics of the metal surface under the coating in a coated metal according to the present invention involves placing the coated metal having a coating and a counter electrode in a solution of a measurement cell. At least three types of DC voltages or currents varying linearly at different rates of change in voltage or current are applied one after another between the coated metal and the counter electrode with a certain de-energized interval between each. Apply the DC voltage or current intermittently and measure the change in the electrolytic current or electrolytic voltage that occurs between the coated metal and the counter electrode due to the applied DC voltage or current, and apply the measured value to the corresponding corresponding voltage for each of the application times. after dividing by the above rate of change, the divided value at the specified rate of change and at least 2
At least two or more subtracted values obtained by mutually subtracting the respective division values at other change rates of the species or more are compared with each other in a relationship corresponding to the respective application times. An apparatus for carrying out a method for measuring external polarization characteristics of a metal surface under a coating film in a coated metal includes a measurement cell formed by immersing a coated metal having a coating film and a counter electrode in a solution;
a means for eliminating the potential difference between the painted metal and the counter electrode; a means for generating direct current or current that changes linearly with at least three or more different voltage or current change rates; At least three types of direct current voltages or currents that vary linearly at different rates of change of voltage or current are applied intermittently one after another between the coated metal and the counter electrode with a certain de-energized interval between each. a means for measuring a change in the electrolytic current or electrolytic voltage generated between the coated metal and the counter electrode due to the DC voltage or current applied by the applying means; A circuit that divides by the corresponding rate of change for each application time, a division value of the division circuit,
A circuit for subtracting the difference between the division value at a specific rate of change and each division value at at least two or more other rates of change, and at least two or more subtraction values obtained by the subtraction circuit, and calculation means for calculating the measured value of the measuring means, which has a circuit that stores the relationship in correspondence with the application time, and therefore, it is possible to apply coating on coated metal using the simple method and simple structure as described above. This method has the advantage that the external polarization characteristics of the metal surface under the film can be easily and reliably measured.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図、イ及びロ、は本発明の定電位法による
測定装置の概略を示す回路図、第2図、イ及び
ロ、は本発明の定電流法による測定方法の概略を
示す回路図、第3図は第1図を具体化したブロツ
ク図、第4図は第3図の具体的な回路図、第5図
は第2図を具体化したブロツク図、第6図は第5
図の具体的な回路図、第7図は第3図と第5図を
1つにまとめた全体の測定装置を示す回路図、第
8図は一つの測定セルの断面図、第9図及び第1
0図は第8図のセルで測定した実験結果の特性
図、第11図は他の測定セルの断面図、第12図
及び第13図は第11図のセルで測定した実験結
果の特性図、第14図及び第15図並びに第16
図は第8図と第11図の実験に関連する特性図、
第17図は本発明の測定方法をデジタル的に処理
する装置のブロツク図、第18図及び第19図は
第17図の装置で測定した実験結果の特性図であ
る。 1…測定セル、W…塗装金属板、R…基準電
極、C…対極、2…電極電位測定手段、3…高入
力抵抗変換器、4…測定準備手段、5…サーボ機
構、6…補償信号供給手段、7…スイツチ、8…
第1演算器、9…比較器、10…サーボモータ、
11…比較信号供給手段、P1〜P2…ポテンシヨ
メータ、R1〜R6…分配抵抗、13…測定装置、
14…直流増巾器、15…多段抵抗器、16…シ
ンクロナスモータ、17…変位コントロール手
段、18…割り算回路、19…直流増巾器、20
…多段抵抗器、21…スイツチ、22…第1記憶
回路、23…第2記憶回路、24…差検出器、2
5…記憶装置。
1, A and B are circuit diagrams schematically showing a measuring device using the constant potential method of the present invention; FIG. 2, A and B are circuit diagrams showing an outline of the measuring method using the constant current method of the present invention; Figure 3 is a block diagram embodying Figure 1, Figure 4 is a concrete circuit diagram of Figure 3, Figure 5 is a block diagram embodying Figure 2, and Figure 6 is a concrete circuit diagram of Figure 5.
7 is a circuit diagram showing the entire measuring device that combines FIGS. 3 and 5 into one, FIG. 8 is a sectional view of one measurement cell, and FIGS. 1st
Figure 0 is a characteristic diagram of the experimental results measured with the cell in Figure 8, Figure 11 is a cross-sectional view of another measurement cell, and Figures 12 and 13 are characteristic diagrams of the experimental results measured with the cell in Figure 11. , Figures 14 and 15, and Figure 16
The figure is a characteristic diagram related to the experiments in Figures 8 and 11,
FIG. 17 is a block diagram of an apparatus for digitally processing the measuring method of the present invention, and FIGS. 18 and 19 are characteristic diagrams of experimental results measured with the apparatus of FIG. 17. DESCRIPTION OF SYMBOLS 1... Measuring cell, W... Painted metal plate, R... Reference electrode, C... Counter electrode, 2... Electrode potential measuring means, 3... High input resistance converter, 4... Measurement preparation means, 5... Servo mechanism, 6... Compensation signal Supply means, 7... Switch, 8...
1st computing unit, 9... comparator, 10... servo motor,
11... Comparison signal supply means, P1 to P2 ... Potentiometer, R1 to R6 ... Distribution resistor, 13... Measuring device,
14... DC amplifier, 15... Multistage resistor, 16... Synchronous motor, 17... Displacement control means, 18... Division circuit, 19... DC amplifier, 20
...Multi-stage resistor, 21...Switch, 22...First memory circuit, 23...Second memory circuit, 24...Difference detector, 2
5...Storage device.

Claims (1)

【特許請求の範囲】 1 塗膜を有する塗装金属と対極とを測定セルの
溶液中に浸漬し、夫々異なる電圧又は電流の変化
率で直線的に変化する少くとも3種以上の直流電
圧又は電流を各々の間に一定の非通電間隔をおい
て上記塗装金属と対極間に次々と断続的に印加し
て、該印加直流電圧又は電流によつて上記塗装金
属と対極間に生じる電解電流又は電解電圧の変化
を測定し、かつ該測定値を上記各印加時間毎に
夫々対応する該当の上記変化率で除算してのち、
特定の変化率における該除算値と少くとも2種以
上の他の変化率における夫々の除算値とを互に減
算して得た少くとも2種以上の減算値を夫々の上
記印加時間と対応した関係で相互に比較させるよ
うにしたことを特徴とする塗装金属における塗膜
下金属面の外部分極特性の測定方法。 2 塗膜を有する塗装金属と対極とを溶液中に浸
漬してなる測定セルと、上記塗装金属と対極との
間の電位差をなくする手段と、少くとも3種以上
の異なる電圧の変化率で直線的に変化する直流電
圧を発生する手段と、該発生手段で発生した夫々
異なる電圧の変化率で直線的に変化する少くとも
3種以上の直流電圧を各々の間に一定の非通電間
隔をおいて上記塗装金属と対極間に次々と断続的
に印加する手段と、該印加手段で印加した直流電
圧によつて上記塗装金属と対極間に生じる電解電
流の変化を測定する手段と、かつ少くとも該測定
手段の測定値を上記各印加時間毎に夫々対応する
該当の上記変化率で除算する回路、該除算回路の
除算値で、特定の変化率における該除算値と少く
とも2種以上の他の変化率における夫々の除算値
の間の差を減算する回路及び該減算回路で得た少
くとも2種以上の減算値を夫々の上記印加時間を
対応させた関係で記憶する回路を持つ上記測定手
段の測定値の演算手段とを備えて成る塗装金属に
おける塗膜下金属面の外部分極特性の測定装置。 3 塗膜を有する塗装金属と対極とを溶液中に浸
漬してなる測定セルと、上記塗装金属と対極との
間の電位差をなくする手段と、少くとも3種以上
の異なる電圧の変化率で直線的に変化する電流を
発生する手段と、該発生手段で発生した夫々異な
る電流の変化率で直線的に変化する少くとも3種
以上の直流電流を各々の間に一定の非通電間隔を
おいて上記塗装金属と対極間に次々と断続的に印
加する手段と、該印加手段で印加した直流電流に
よつて上記塗装金属と対極間に生じる電解電圧の
変化を測定する手段と、かつ少くとも該測定手段
の測定値を上記各印加時間毎に夫々対応する該当
の上記変化率で除算する回路、該除算回路の除算
値で、特定の変化率における該除算値と少くとも
2種以上の他の変化率における夫々の除算値の間
の差を減算する回路及び該減算回路で得た少くと
も2種以上の減算値を夫々の上記印加時間と対応
させた関係で記憶する回路を持つ上記測定手段の
測定値の演算手段とを備えて成る塗装金属におけ
る塗膜下金属面の外部分極特性の測定装置。
[Scope of Claims] 1. A coated metal having a coating film and a counter electrode are immersed in a solution of a measurement cell, and at least three or more types of DC voltages or currents are applied, each of which varies linearly at a different rate of change of voltage or current. is applied intermittently between the coated metal and the counter electrode with a certain non-current interval between each, and the electrolytic current or electrolysis generated between the coated metal and the counter electrode due to the applied DC voltage or current is After measuring the change in voltage and dividing the measured value by the corresponding rate of change for each application time,
At least two or more subtracted values obtained by mutually subtracting the division value at a specific rate of change and each division value at at least two other rates of change correspond to each of the above application times. A method for measuring external polarization characteristics of a metal surface under a coating film in a coated metal, characterized in that the characteristics are compared with each other based on the relationship. 2. A measuring cell comprising a coated metal having a coating film and a counter electrode immersed in a solution, a means for eliminating the potential difference between the coated metal and the counter electrode, and at least three or more different voltage change rates. A means for generating a DC voltage that varies linearly, and at least three types of DC voltages that vary linearly at different rates of change of voltage generated by the generating means, each with a fixed non-energizing interval between each. a means for applying an electrolytic current intermittently between the coated metal and the counter electrode one after another; a means for measuring changes in electrolytic current generated between the coated metal and the counter electrode due to the DC voltage applied by the applying means; A circuit that divides the measured value of the measuring means by the corresponding rate of change for each application time, and a division value of the division circuit that is at least two or more different from the division value at a specific rate of change. The above-mentioned device has a circuit for subtracting the difference between the respective division values at other rates of change, and a circuit for storing at least two or more types of subtraction values obtained by the subtraction circuit in a relationship that corresponds to each of the above-mentioned application times. 1. A measuring device for measuring external polarization characteristics of a metal surface under a coating film in a coated metal, comprising a measuring means and a calculating means for calculating a measured value. 3. A measurement cell comprising a coated metal having a coating film and a counter electrode immersed in a solution, a means for eliminating the potential difference between the coated metal and the counter electrode, and at least three or more different voltage change rates. A means for generating a current that varies linearly, and at least three types of direct current that vary linearly at different rates of change of current generated by the generating means, each with a fixed non-energizing interval between them. means for intermittently applying a direct current between the coated metal and the counter electrode, and a means for measuring changes in electrolytic voltage generated between the coated metal and the counter electrode due to the direct current applied by the applying means, and at least a circuit that divides the measured value of the measuring means by the corresponding rate of change for each application time; The above measurement has a circuit for subtracting the difference between the respective division values in the rate of change of and a circuit for storing at least two or more subtracted values obtained by the subtraction circuit in a relationship corresponding to the respective application times. and a calculation means for calculating the measured value of the means.
JP15682280A 1980-11-06 1980-11-06 Method and apparatus for measuring outer polarization characteristics of metal surface under film of coating metal Granted JPS5780551A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15682280A JPS5780551A (en) 1980-11-06 1980-11-06 Method and apparatus for measuring outer polarization characteristics of metal surface under film of coating metal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15682280A JPS5780551A (en) 1980-11-06 1980-11-06 Method and apparatus for measuring outer polarization characteristics of metal surface under film of coating metal

Publications (2)

Publication Number Publication Date
JPS5780551A JPS5780551A (en) 1982-05-20
JPS6322257B2 true JPS6322257B2 (en) 1988-05-11

Family

ID=15636096

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15682280A Granted JPS5780551A (en) 1980-11-06 1980-11-06 Method and apparatus for measuring outer polarization characteristics of metal surface under film of coating metal

Country Status (1)

Country Link
JP (1) JPS5780551A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5948649A (en) * 1982-09-13 1984-03-19 Nippon Paint Co Ltd Method and apparatus for corrosion resistance evaluation of painted metal
JPH0619339B2 (en) * 1986-10-01 1994-03-16 日本ペイント株式会社 Highly sensitive polarization measuring method and apparatus for coated metal

Also Published As

Publication number Publication date
JPS5780551A (en) 1982-05-20

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