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JPH077004B2 - Accuracy measurement method of rotation unevenness measuring device - Google Patents
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JPH077004B2 - Accuracy measurement method of rotation unevenness measuring device - Google Patents

Accuracy measurement method of rotation unevenness measuring device

Info

Publication number
JPH077004B2
JPH077004B2 JP32047189A JP32047189A JPH077004B2 JP H077004 B2 JPH077004 B2 JP H077004B2 JP 32047189 A JP32047189 A JP 32047189A JP 32047189 A JP32047189 A JP 32047189A JP H077004 B2 JPH077004 B2 JP H077004B2
Authority
JP
Japan
Prior art keywords
trigger
laser beam
reflected
signals
time difference
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 - Lifetime
Application number
JP32047189A
Other languages
Japanese (ja)
Other versions
JPH03181863A (en
Inventor
宏 中吉
巌 杉崎
克 田代
理絵 若島
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.)
Nidec Copal Electronics Corp
Original Assignee
Copal Electronics 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 Copal Electronics Co Ltd filed Critical Copal Electronics Co Ltd
Priority to JP32047189A priority Critical patent/JPH077004B2/en
Publication of JPH03181863A publication Critical patent/JPH03181863A/en
Publication of JPH077004B2 publication Critical patent/JPH077004B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Mechanical Optical Scanning Systems (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、レーザビームプリンタに用いられるポリゴン
ミラを使った光走査装置の回転ムラ測定装置の精度測定
方法に関するものである。
Description: TECHNICAL FIELD The present invention relates to an accuracy measuring method of a rotation unevenness measuring device of an optical scanning device using a polygon mirror used in a laser beam printer.

(従来の技術) 一般にスキャナモータの回転精度の測定方法は、第2図
に示すように、ポリゴンミラ1に、レーザ光源2により
レーザビームL11を照射し、走査された反射ビームL12
を、ポリゴンミラ1に対して所定の見込角を持って配置
された2つのトリガ発生器13,14で受けることにより、
トリガ信号S1,S2を得る。
(Prior Art) In general, a method of measuring the rotational accuracy of a scanner motor is as shown in FIG. 2, in which a polygon mirror 1 is irradiated with a laser beam L11 from a laser light source 2 and a reflected beam L12 is scanned.
Is received by the two trigger generators 13 and 14 arranged with a predetermined prospective angle with respect to the polygon mirror 1,
Obtain trigger signals S1 and S2.

この原理を、トリガ発生器13について説明すると、第3
図に示すように、走査された反射ビームL12のスポット
Pが、トリガ発生器13の開口部Dを、図の左から右へ通
過するので、開口部Dへの入射光量に応じてアナログ信
号Saが得られる。このアナログ信号Saを所定のレベルSL
と比較して、デジタル化した結果をトリガ信号S1として
出力する。
The principle of the trigger generator 13 will be explained below.
As shown in the figure, the spot P of the scanned reflected beam L12 passes through the opening D of the trigger generator 13 from the left to the right in the figure, so that the analog signal Sa depending on the amount of light incident on the opening D is generated. Is obtained. This analog signal Sa is set to a predetermined level SL
And the digitized result is output as the trigger signal S1.

このようにして得られた2つのトリガ信号S1,S2を時間
差測定手段(例えば、カウンタ)15の入力端子A,Bへ入
力することにより、第4図に示すように反射ビームL12
が2つのトリガ発生器13,14を走査する平均走査時間
t、および変動量Δtが得られ、これにより、ポリゴン
スキャナの回転精度Jが(Δt/t)として求められる。
By inputting the two trigger signals S1 and S2 thus obtained to the input terminals A and B of the time difference measuring means (for example, a counter) 15, the reflected beam L12 as shown in FIG.
The average scanning time t for scanning the two trigger generators 13 and 14 and the fluctuation amount Δt are obtained, whereby the rotation accuracy J of the polygon scanner is obtained as (Δt / t).

(発明が解決しようとする課題) トリガ発生器13,14からの信号S1,S2は、スキャナの回転
変動以外の成分(例えば、トリガを発生するための光電
変換器や回路のノイズ等)を含んでいることが多い。
(Problems to be Solved by the Invention) The signals S1 and S2 from the trigger generators 13 and 14 include components other than rotational fluctuations of the scanner (for example, noise of a photoelectric converter or circuit for generating a trigger). I often go out.

よって、このような測定系では、スキャナの回転変動以
外の成分もデータに含まれてしまうが、これまでは、そ
の成分の定量的な大きさを把握する手段がなかった。
Therefore, in such a measurement system, components other than the rotational fluctuation of the scanner are included in the data, but until now, there was no means for grasping the quantitative magnitude of the component.

(課題を解決するための手段) 本発明は、前記課題を解決するためになされたもので、 回転しているポリゴンミラにレーザ光源によりレーザビ
ームを照射し、走査された反射ビームをポリゴンミラに
対して所定の見込角を持って配置された2つのトリガ発
生器で受けることにより各々トリガ信号を発生させ、前
記トリガ信号をデジタル信号に変換して時間差測定手段
に入力し、2つのトリガ信号間の平均走査時間及び変動
量から、ポリゴンスキャナの回転精度を測定する回転ム
ラ測定装置において、 回転しているポリゴンミラ1にレーザ光源2から出射さ
れたレーザビームL1を入射し、その反射されたレーザビ
ームL2がハーフミラ5を通過し、その通過したレーザビ
ームLaがトリガ発生器4へ入射してトリガ信号を発生さ
せ、同時にハーフミラ5で反射したレーザビームLbがも
う一つのトリガ発生器3へ入射してトリガ信号を発生さ
せるように、ハーフミラ5、トリガ発生器4,3を近接さ
せて配置し、前記トリガ発生器4,3のトリガ信号を各々
デジタル信号に変換して時間差測定手段に入力し、2つ
のトリガ信号間の時間差及び変動量を測定するようにし
たものである。
(Means for Solving the Problems) The present invention has been made to solve the above problems, and a rotating polygon mirror is irradiated with a laser beam from a laser light source, and a scanned reflected beam is applied to the polygon mirror. On the other hand, two trigger generators arranged at a predetermined angle of view generate trigger signals respectively, and the trigger signals are converted into digital signals and input to the time difference measuring means, between the two trigger signals. In a rotation unevenness measuring device that measures the rotation accuracy of a polygon scanner from the average scanning time and fluctuation amount of the laser beam L1 emitted from the laser light source 2 to the rotating polygon mirror 1, the reflected laser beam is reflected. The beam L2 passes through the half mirror 5, and the passed laser beam La is incident on the trigger generator 4 to generate a trigger signal, and at the same time, the half mirror 5 is generated. The half mirror 5 and the trigger generators 4 and 3 are arranged close to each other so that the laser beam Lb reflected by the laser beam 5 enters the other trigger generator 3 to generate a trigger signal. Each of the trigger signals is converted into a digital signal and input to the time difference measuring means to measure the time difference between the two trigger signals and the variation amount.

(作用) 本発明によれば、通過したレーザビームLaと反射したレ
ーザビームLbが同時にトリガ発生器4,3へ入射するよう
に光学系を配置し、トリガ発生器4,3からのトリガ信号
をデジタル信号に変換して時間差測定手段に入力し、2
つのトリガ信号間の時間差及び変動量を測定することに
より、回転ムラ測定装置の測定データに含まれる、ポリ
ゴンミラ1の回転変動以外の成分を定量的に評価するこ
とができる。
(Operation) According to the present invention, the optical system is arranged so that the passed laser beam La and the reflected laser beam Lb are simultaneously incident on the trigger generators 4 and 3, and the trigger signals from the trigger generators 4 and 3 are generated. Convert it to a digital signal and input it to the time difference measuring means
By measuring the time difference between the two trigger signals and the fluctuation amount, it is possible to quantitatively evaluate the components other than the rotation fluctuation of the polygon mirror 1 included in the measurement data of the rotation unevenness measuring device.

(実施例) 第1図は、本発明の一実施例を説明する図であって、レ
ーザ光源2から出射されたレーザビームL1をポリゴンミ
ラ1へ入射し、その反射したレーザビームL2は、ポリゴ
ンミラ1の矢印方向への回転に伴って走査され、所定の
位置においてハーフミラ5へ入射し、通過したレーザビ
ームLaと反射したレーザビームLbに分けられる。この場
合、レーザビームLa,Lbの各々がトリガ発生器4,3へ同時
に入射するようにハーフミラ5と、トリガ発生器4,3を
近接して配置する。このようにして得られたトリガ発生
器4,3よりのトリガ信号(図示せず)の時間差及び変動
量を、第2図で示した時間差測定手段(例えば、カウン
タ)15で測定する。
(Embodiment) FIG. 1 is a diagram for explaining an embodiment of the present invention, in which a laser beam L1 emitted from a laser light source 2 is incident on a polygon mirror 1 and the reflected laser beam L2 is a polygon. Scanning is performed as the mirror 1 rotates in the direction of the arrow, and the laser beam La is incident on the half mirror 5 at a predetermined position and is divided into a laser beam La that has passed and a laser beam Lb that has been reflected. In this case, the half mirror 5 and the trigger generators 4 and 3 are arranged close to each other so that the laser beams La and Lb respectively enter the trigger generators 4 and 3 at the same time. The time difference and the amount of fluctuation of the trigger signals (not shown) from the trigger generators 4 and 3 thus obtained are measured by the time difference measuring means (for example, counter) 15 shown in FIG.

この時、通過したレーザビームLaと反射したレーザビー
ムLbが同時にトリガ発生器4,3へ入射するように光学系
を配置しているので、実際にレーザビームを走査して測
定された、2つのトリガ信号間の時間差及び変動量は、
すなわち、回転ムラ測定装置の誤差(例えば、トリガを
発生するための光電変換器や回路のノイズ等によるも
の)である。
At this time, since the optical system is arranged so that the passed laser beam La and the reflected laser beam Lb are simultaneously incident on the trigger generators 4 and 3, two laser beams actually measured by scanning the laser beam are measured. The time difference between trigger signals and the amount of fluctuation are
That is, it is an error of the rotation unevenness measuring apparatus (for example, due to noise of a photoelectric converter or circuit for generating a trigger).

なぜならば、ハーフミラ5、トリガ発生器4、およびト
リガ発生器3は近接して配置されているため、それらを
固定した光学系の歪などの影響は無視でき、同一のレー
ザビームが同時にトリガ発生器に照射され、このレーザ
ビームによりトリガ信号を得るように構成されているた
め、ポリゴンミラ1の回転変動は測定量に入ってこない
ためである。
Because the half mirror 5, the trigger generator 4, and the trigger generator 3 are arranged close to each other, the influence of the distortion of the optical system fixing them can be ignored, and the same laser beam is simultaneously generated by the trigger generator. This is because the rotation fluctuation of the polygon mirror 1 does not enter the measurement amount because the laser beam is irradiated to the laser beam and the trigger signal is obtained by this laser beam.

(発明の効果) 以上、詳細に説明したように、本発明によれば、ポリゴ
ンミラの回転変動以外の測定系の誤差を定量的に評価す
ることができる、すなわち、ポリゴンミラの回転ムラ測
定装置に含まれる、トリガ発生器周辺の誤差を定量的に
評価することにより、回転ムラ測定装置の精度を測定す
ることが可能となる。このため、ポリゴンミラの回転ム
ラを、より正確に求めることができる。
(Effects of the Invention) As described above in detail, according to the present invention, it is possible to quantitatively evaluate the error of the measurement system other than the rotation fluctuation of the polygon mirror, that is, the rotation unevenness measuring apparatus for the polygon mirror. It is possible to measure the accuracy of the rotation unevenness measuring apparatus by quantitatively evaluating the error around the trigger generator included in the above. Therefore, the rotation irregularity of the polygon mirror can be obtained more accurately.

【図面の簡単な説明】[Brief description of drawings]

第1図は、本発明の一実施例を示す構成図、第2図は、
スキャナモータの回転精度測定装置の構成図、第3図
は、トリガ発生器の原理を説明する図、第4図は、デジ
タル化したトリガ信号を示す図である。 1……ポリゴンミラ 2……レーザ光源 3,4,13,14……トリガ発生器 5……ハーフミラ 15……時間差測定手段
FIG. 1 is a block diagram showing an embodiment of the present invention, and FIG.
FIG. 3 is a configuration diagram of a rotation accuracy measuring device of a scanner motor, FIG. 3 is a diagram for explaining the principle of a trigger generator, and FIG. 4 is a diagram showing a digitized trigger signal. 1 …… Polygon mirror 2 …… Laser light source 3,4,13,14 …… Trigger generator 5 …… Half mirror 15 …… Time difference measuring means

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】回転しているポリゴンミラにレーザ光源に
よりレーザビームを照射し、走査された反射ビームをポ
リゴンミラに対して所定の見込角を持って配置された2
つのトリガ発生器で受けることにより各々トリガ信号を
発生させ、前記トリガ信号をデジタル信号に変換して時
間差測定手段に入力し、2つのトリガ信号間の平均走査
時間及び変動量から、ポリゴンスキャナの回転精度を測
定する回転ムラ測定装置において、 回転しているポリゴンミラ(1)にレーザ光源(2)か
ら出射されたレーザビーム(L1)を入射し、その反射さ
れたレーザビーム(L2)がハーフミラ(5)を通過し、
その通過したレーザビーム(La)がトリガ発生器(4)
へ入射してトリガ信号を発生させ、同時にハーフミラ
(5)で反射したレーザビーム(Lb)がもう一つのトリ
ガ発生器(3)へ入射してトリガ信号を発生させるよう
に、ハーフミラ(5)、トリガ発生器(4),(3)を
近接させて配置し、前記トリガ発生器(4),(3)の
トリガ信号を各々デジタル信号に変換して時間差測定手
段に入力し、2つのトリガ信号間の時間差及び変動量を
測定することを特徴とする回転ムラ測定装置の精度測定
方法。
1. A rotating polygon mirror is irradiated with a laser beam from a laser light source, and a reflected beam scanned is arranged at a predetermined angle with respect to the polygon mirror.
The trigger signals are generated by being received by two trigger generators, the trigger signals are converted into digital signals and input to the time difference measuring means, and the rotation of the polygon scanner is determined based on the average scanning time and fluctuation amount between the two trigger signals. In a rotation unevenness measuring device for measuring accuracy, a laser beam (L1) emitted from a laser light source (2) is incident on a rotating polygon mirror (1), and the reflected laser beam (L2) is reflected by a half mirror (1). Go through 5),
The passed laser beam (La) is a trigger generator (4)
To generate a trigger signal, and at the same time, the laser beam (Lb) reflected by the half mirror (5) enters another trigger generator (3) to generate a trigger signal. The trigger generators (4) and (3) are arranged close to each other, and the trigger signals of the trigger generators (4) and (3) are respectively converted into digital signals and input to the time difference measuring means, and two trigger signals are provided. An accuracy measuring method for a rotation unevenness measuring device, characterized by measuring a time difference between the two and a fluctuation amount.
JP32047189A 1989-12-12 1989-12-12 Accuracy measurement method of rotation unevenness measuring device Expired - Lifetime JPH077004B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32047189A JPH077004B2 (en) 1989-12-12 1989-12-12 Accuracy measurement method of rotation unevenness measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32047189A JPH077004B2 (en) 1989-12-12 1989-12-12 Accuracy measurement method of rotation unevenness measuring device

Publications (2)

Publication Number Publication Date
JPH03181863A JPH03181863A (en) 1991-08-07
JPH077004B2 true JPH077004B2 (en) 1995-01-30

Family

ID=18121822

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32047189A Expired - Lifetime JPH077004B2 (en) 1989-12-12 1989-12-12 Accuracy measurement method of rotation unevenness measuring device

Country Status (1)

Country Link
JP (1) JPH077004B2 (en)

Also Published As

Publication number Publication date
JPH03181863A (en) 1991-08-07

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