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JPS6340324B2 - - Google Patents
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JPS6340324B2 - - Google Patents

Info

Publication number
JPS6340324B2
JPS6340324B2 JP4451181A JP4451181A JPS6340324B2 JP S6340324 B2 JPS6340324 B2 JP S6340324B2 JP 4451181 A JP4451181 A JP 4451181A JP 4451181 A JP4451181 A JP 4451181A JP S6340324 B2 JPS6340324 B2 JP S6340324B2
Authority
JP
Japan
Prior art keywords
electrolyte
electrode
copper ion
ion conductor
present
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
JP4451181A
Other languages
Japanese (ja)
Other versions
JPS57158904A (en
Inventor
Satoshi Sekido
Yoshito Ninomya
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP56044511A priority Critical patent/JPS57158904A/en
Publication of JPS57158904A publication Critical patent/JPS57158904A/en
Publication of JPS6340324B2 publication Critical patent/JPS6340324B2/ja
Granted legal-status Critical Current

Links

Classifications

    • Y02E60/12

Landscapes

  • Conductive Materials (AREA)
  • Primary Cells (AREA)

Description

【発明の詳細な説明】 本発明は室温附近で高いイオン導電性を有し、
しかも電子輸率が小さく安定な銅イオン導電体と
その製造法を提供するものである。
[Detailed description of the invention] The present invention has high ionic conductivity near room temperature,
Furthermore, the present invention provides a stable copper ion conductor with a small electron transport number and a method for producing the same.

従来、室温で高いイオン導電性を示す物質とし
てAgIを部分的にアニオン、カチオン、あるいは
アニオン・カチオン混合置換した銀イオン導電体
がある。これを用いた電池、電気二重層キヤパシ
タ、WO3を用いたデイスプレイ素子も開発され
ているが、材料的に銀および銀塩を主体として構
成されるためにどうしても高価となり、余り普及
して居なかつた。
Conventionally, there are silver ion conductors in which AgI is partially substituted with anions, cations, or mixed anions and cations as substances that exhibit high ionic conductivity at room temperature. Batteries using this material, electric double layer capacitors, and display elements using WO 3 have also been developed, but since they are mainly composed of silver and silver salts, they are expensive and have not become very popular. Ta.

これに対して銅イオン導電体を用いようとする
試みもなされているが、今までに得られた高いイ
オン導電性を示す物質は、有機物質を用いている
ので耐熱性が低かつたり、高温で電子導電性が高
くなつたりして実用温度領域が狭い欠点があつ
た。
In response, attempts have been made to use copper ion conductors, but the materials that have been obtained so far that exhibit high ionic conductivity have low heat resistance or high temperature because they use organic materials. However, it had the disadvantage of having a narrow practical temperature range due to its high electronic conductivity.

発明者らは、これに対してCuClのCu+イオンの
1/5をRb+、K+、NH4 +、NR4 +で、Cl-イオンの
1/3〜1/4をI-イオンで混合置換した物質が室温で
比較的高いCu+イオン導電性を示し、実用温度範
囲も比較的広いことを既に見出した。
In contrast, the inventors found that 1/5 of the Cu + ions in CuCl are Rb + , K + , NH 4 + , and NR 4 + , and 1/3 to 1/4 of the Cl - ions are I - ions. We have already found that the mixed-substituted materials exhibit relatively high Cu + ion conductivity at room temperature and have a relatively wide practical temperature range.

本発明は、Cu+イオンの置換をRb+、K+
NH4 +、NR4 +イオン単独で行なうよりRb+とK+
との2種類のカチオンで置換した方がさらにイオ
ン導電率が高く、電池などのデバイスに用いても
内部抵抗が低くでき、さらに大きな電流が流せる
ことができることを見出したことに基づいてなさ
れたものである。
The present invention replaces Cu + ions with Rb + , K + ,
Rb + and K + than NH 4 + , NR 4 + ions alone
This was based on the discovery that replacing cations with two types of cations has higher ionic conductivity, lowers internal resistance when used in devices such as batteries, and allows even larger currents to flow. It is.

以下に図面を用いて本発明の実施例を説明す
る。予め140℃で空気中で2hr加熱したKCl、
RbCl、CuCl、CuIをMeCu4I1.5Cl3.5の割り合いで
乳鉢で混合した。MeとしてRbだけのもの(従
来)とKおよびRbの混合物(本発明)を用いた。
これらの混合物をプレス成型してペレツトにした
ものをガラス製密封容器に入れ、内部を真空に引
いた後、250℃で17hr加熱し反応させた。生成物
のX線回折をとると、第1図のように原材料と全
く異なる物質が生成しており、それは結晶として
は従来のRbCu4I1.5Cl3.5と同じ構造に属すること
が認められた。また、組成と格子定数および室温
導電率との関係は第2図のようになりKの添加に
より格子定数は小さくなり、導電率は本発明の組
成領域で5割程度低くなつた。電子輸率は従来同
様に極めて低いから、導電率の増大はイオン導電
率の増大によることは明らかである。
Embodiments of the present invention will be described below with reference to the drawings. KCl, pre-heated at 140 °C for 2 hr in air
RbCl, CuCl, and CuI were mixed in a mortar at a ratio of MeCu 4 I 1.5 Cl 3.5 . As Me, only Rb (conventional) and a mixture of K and Rb (invention) were used.
These mixtures were press-molded into pellets, placed in a sealed glass container, the inside of which was evacuated, and then heated at 250° C. for 17 hours to cause a reaction. When the product was subjected to X-ray diffraction, a substance completely different from the raw material was formed as shown in Figure 1, and it was confirmed that this crystal had the same structure as the conventional RbCu 4 I 1.5 Cl 3.5 . Further, the relationship between the composition, lattice constant, and room temperature conductivity is as shown in FIG. 2, and the addition of K reduces the lattice constant and the conductivity decreases by about 50% in the composition range of the present invention. Since the electron transport number is extremely low as in the conventional case, it is clear that the increase in electrical conductivity is due to the increase in ionic conductivity.

次に本発明による電解質を電気化学デバイスと
しての電気二重層容量応用素子に用いた場合の効
果を示す。電気二重層容量応用素子の構成を第3
図に示す。図において1は分極性電極で材料とし
てはカーボン、Cu2Sのように電子導電性をもち、
電気化学的に不活性な物質と電解質との混合成型
物からなる電極である。電極材料による違いは次
の通りである。カーボン、白金、パラジウムなど
は電解質の分解電圧(約0.6V)以内の電圧範囲
での通電によつて電極で電気化学反応が起らず、
電解質の分解電圧が耐圧となり得るが、吸着した
ガスが耐圧以下でも電気化学反応を行なうので、
除去に留意しないとリーク電流となつて表われ
る。Cu2Sはリーク電流は少ないが、電気化学反
応を行わない電圧範囲が0.07Vと狭い欠点があ
る。2は分極性電極1の集電体で、グラフアイ
ト、白金、パラジウム、金を蒸着、またはスパツ
タで形成する。3は電解質である。4は対極で
Cu2SとCuとの2:3混合物、TiS2とCuとの3:
7混合物、あるいはCu2S単独と電解質との混合
物である。これらは非分極性電極と称するもの
で、Cu+イオンの析出・溶解反応が通電によつて
行われる。混合物電極は開路電圧がCuのそれに
近いもので、Cu電極よりも可逆性に優れている。
またCu2S単独のものはそれより310mV貴の開路
電圧を示す点が異なる。5は対極4の集電体で銅
をネツトとして対極4に圧入するか、対極4上に
蒸着する。6は電解質、7は基準極でCu2Sと電
解質との混合物を用いた。8は基準極7の集電体
で銅を用いている。なお電解質6、基準極7、集
電体8は各電極の電位変化を正確に測定するため
に設けたもので、出力を得るためのキヤパシタに
は不必要である。
Next, the effects when the electrolyte according to the present invention is used in an electric double layer capacitance applied element as an electrochemical device will be described. The third configuration of the electric double layer capacitance applied element
As shown in the figure. In the figure, 1 is a polarizable electrode, and the material is carbon, which has electronic conductivity like Cu 2 S.
An electrode made of a molded mixture of an electrochemically inert substance and an electrolyte. The differences depending on the electrode material are as follows. Carbon, platinum, palladium, etc. do not cause an electrochemical reaction at the electrode when energized within the voltage range of the electrolyte decomposition voltage (approximately 0.6V).
The decomposition voltage of the electrolyte can be a withstand voltage, but the adsorbed gas will undergo an electrochemical reaction even below the withstand voltage.
If care is not taken to remove it, it will appear as a leakage current. Although Cu 2 S has low leakage current, it has the disadvantage that the voltage range in which electrochemical reactions do not occur is narrow at 0.07V. Reference numeral 2 denotes a current collector for the polarizable electrode 1, which is formed of graphite, platinum, palladium, or gold by vapor deposition or sputtering. 3 is an electrolyte. 4 is the opposite
2 :3 mixture of Cu2S and Cu, 3:3 of TiS2 and Cu
7 mixture, or a mixture of Cu 2 S alone and an electrolyte. These are called non-polarizable electrodes, and the precipitation and dissolution reactions of Cu + ions are carried out by applying electricity. The mixture electrode has an open circuit voltage close to that of Cu and has better reversibility than the Cu electrode.
The difference is that Cu 2 S alone exhibits an open circuit voltage of 310 mV higher than that. Reference numeral 5 denotes a current collector for the counter electrode 4, and the copper is either press-fitted into the counter electrode 4 as a net or deposited on the counter electrode 4 by vapor deposition. 6 is an electrolyte, and 7 is a reference electrode, in which a mixture of Cu 2 S and an electrolyte is used. 8 is a current collector of the reference electrode 7, which is made of copper. Note that the electrolyte 6, the reference electrode 7, and the current collector 8 are provided to accurately measure potential changes of each electrode, and are not necessary for a capacitor for obtaining an output.

分極性電極1にCu2S、対極4にCu2SとCuとの
混合物を用い、分極性電極1の重量0.1g、その
他の電極と電解質を0.2g採取して10mmφの円筒
状素子とした。第4図、第5図は、電解質に本発
明による電解質を採用した場合(図中領域Aに示
す)と、比較のための電解質を用いた場合(図中
領域Bに示す)のそれぞれの特性を示す。第4図
は分極性電極の通電々流による電位変化と通電停
止後の電位変化を示したものである。従来の電解
質を用いた場合は20mAの通電になると電解質中
のイオンの移動の遅れと考えられる電位変化が起
り、電位上昇の遅れa、通電停止後の電位のオー
バーシユートbと低下cが大きくなつたが本発明
による電解質を用いたものはそのようなことが起
らず30mA通電になつてはじめて起つた。
Using Cu 2 S for polarizable electrode 1 and a mixture of Cu 2 S and Cu for counter electrode 4, 0.1 g of polarizable electrode 1 and 0.2 g of other electrodes and electrolyte were collected to form a 10 mmφ cylindrical element. . Figures 4 and 5 show the respective characteristics when the electrolyte according to the present invention is used as the electrolyte (shown in area A in the figure) and when an electrolyte for comparison is used (shown in area B in the figure). shows. FIG. 4 shows the potential change due to current flow of the polarizable electrode and the potential change after the current supply is stopped. When a conventional electrolyte is used, when a current of 20 mA is applied, a potential change occurs, which is thought to be due to a delay in the movement of ions in the electrolyte, and there is a delay in potential rise (a), and a large overshoot (b) and decrease (c) in the potential after the current is stopped. When Natsuta used the electrolyte according to the present invention, such a problem did not occur, but only after 30 mA of current was applied.

対極の電位変化は第5図のようになり、本発明
による電解質を用いると分極がいちじるしく小さ
くなつた。対極の分極が無視できれば、基準極を
用いずに2極構成の素子でも端子電圧によつて分
極性電極の電位挙動を示すことができ、分極性電
極の通電々気量に対する電位の直線性と通電停止
時の電位の保持を利用する電位記憶素子の構成が
簡単になるとか、あるいは電気エネルギの蓄積、
放出用キヤパシタとして用いる場合も損失エネル
ギを少なくすることができる利点がある。
The potential change of the counter electrode was as shown in FIG. 5, and the polarization was significantly reduced by using the electrolyte according to the present invention. If the polarization of the opposite electrode can be ignored, even a device with a two-pole configuration can show the potential behavior of the polarizable electrode depending on the terminal voltage without using a reference electrode, and the linearity of the potential with respect to the current flow rate of the polarizable electrode It is possible to simplify the configuration of a potential storage element that uses potential retention when power is stopped, or to store electrical energy.
When used as a discharge capacitor, it also has the advantage of reducing energy loss.

なお、前記実施例においては本発明による電解
質を電気二重層キヤパシタ用いた場合について示
したが、電池およびWO3を用いる電気化学的デ
イスプレイ装置においても、違いは分極性電極を
使うことなく、両電極とも非分極性電極を使うだ
けであるから、通電による損失を少なくすること
ができる効果において全く同じである。
In the above example, the case where the electrolyte according to the present invention is used in an electric double layer capacitor is shown, but the difference is that the electrolyte according to the present invention is used in an electric double layer capacitor. Since both use only non-polarizable electrodes, they have exactly the same effect of reducing loss due to current flow.

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

第1図は従来の銅イオン導電体(RbCu4I1.5
Cl3.5)との比較の上で示した本発明による銅イオ
ン導電体のX線回折図、第2図は本発明による銅
イオン導電体の格子定数および導電率を示す図、
第3図は銅イオン導電体を電解質として用いた電
気二重層容量応用素子の構成を示す断面図、第4
図は本発明による銅イオン導電体および従来の銅
イオン導電体をそれぞれ電解質として用いた電気
二重層容量応用素子の分極性電極の電位変化を示
す図、第5図は同電気二重層容量応用素子の対極
の電位変化を示す図である。 1……分極性電極、3,6……電解質、4……
対極、7……基準極。
Figure 1 shows a conventional copper ion conductor (RbCu 4 I 1.5
An X-ray diffraction diagram of the copper ion conductor according to the present invention shown in comparison with Cl 3.5 ), FIG. 2 is a diagram showing the lattice constant and conductivity of the copper ion conductor according to the present invention,
Figure 3 is a cross-sectional view showing the configuration of an electric double layer capacitance applied element using a copper ion conductor as an electrolyte;
The figure shows the potential change of the polarizable electrode of an electric double layer capacitance application device using the copper ion conductor according to the present invention and the conventional copper ion conductor as electrolytes, and Fig. 5 shows the same electric double layer capacitance application device. It is a figure which shows the potential change of the counter electrode of. 1... Polarizable electrode, 3, 6... Electrolyte, 4...
Opposite pole, 7...Reference pole.

Claims (1)

【特許請求の範囲】 1 化学式MeCu4I2-xCl3+x(0.25x0.5)で表
わされる化合物において上記Meが1:9〜1:
3のKとRbとからなる化合物を用いることを特
徴とする銅イオン導電体。 2 化学式MeCu4I2-xCl3+x(0.25x0.5)で表
わされる化合物において上記Meが1:9〜1:
3のKとRbとからなる化合物を用いる銅イオン
導電体の製造法において、KCl、RbCl、CuCl、
CuIを所定の割り合いで混合し、加圧成型したペ
レツトを密封容器に入れ、内部を真空にした後、
加熱反応せしめることにより上記化合物を得るこ
とを特徴とする銅イオン導電体の製造法。 3 ペレツトを200〜300℃の温度で加熱すること
を特徴とする特許請求の範囲第2項記載の銅イオ
ン導電体の製造法。
[Claims] 1. In the compound represented by the chemical formula MeCu 4 I 2-x Cl 3+x (0.25x0.5), the above Me is 1:9 to 1:
A copper ion conductor characterized by using a compound consisting of K and Rb in No. 3. 2 In the compound represented by the chemical formula MeCu 4 I 2-x Cl 3+x (0.25x0.5), the above Me is 1:9 to 1:
In the method for producing a copper ion conductor using a compound consisting of K and Rb in No. 3, KCl, RbCl, CuCl,
After mixing CuI at a predetermined ratio and press-molding the pellets into a sealed container and evacuating the inside,
A method for producing a copper ion conductor, characterized in that the above compound is obtained by a heating reaction. 3. The method for producing a copper ion conductor according to claim 2, characterized in that the pellets are heated at a temperature of 200 to 300°C.
JP56044511A 1981-03-25 1981-03-25 Copper ion conductor and method of producing same Granted JPS57158904A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56044511A JPS57158904A (en) 1981-03-25 1981-03-25 Copper ion conductor and method of producing same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56044511A JPS57158904A (en) 1981-03-25 1981-03-25 Copper ion conductor and method of producing same

Publications (2)

Publication Number Publication Date
JPS57158904A JPS57158904A (en) 1982-09-30
JPS6340324B2 true JPS6340324B2 (en) 1988-08-10

Family

ID=12693569

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56044511A Granted JPS57158904A (en) 1981-03-25 1981-03-25 Copper ion conductor and method of producing same

Country Status (1)

Country Link
JP (1) JPS57158904A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6394121U (en) * 1986-12-08 1988-06-17

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6394121U (en) * 1986-12-08 1988-06-17

Also Published As

Publication number Publication date
JPS57158904A (en) 1982-09-30

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