JPH0342617Y2 - - Google Patents

Info

Publication number
JPH0342617Y2
JPH0342617Y2 JP1984007472U JP747284U JPH0342617Y2 JP H0342617 Y2 JPH0342617 Y2 JP H0342617Y2 JP 1984007472 U JP1984007472 U JP 1984007472U JP 747284 U JP747284 U JP 747284U JP H0342617 Y2 JPH0342617 Y2 JP H0342617Y2
Authority
JP
Japan
Prior art keywords
magnetic field
coil
excitation coil
current
power source
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
JP1984007472U
Other languages
Japanese (ja)
Other versions
JPS60121253U (en
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 filed Critical
Priority to JP747284U priority Critical patent/JPS60121253U/en
Publication of JPS60121253U publication Critical patent/JPS60121253U/en
Application granted granted Critical
Publication of JPH0342617Y2 publication Critical patent/JPH0342617Y2/ja
Granted legal-status Critical Current

Links

Description

【考案の詳細な説明】 本考案は分析用磁場を発生する電磁石装置を備
えた質量分析装置に関し、特に外部から到来する
外来磁力線により生じる比較的周波数の高い磁場
変動を除くことのできる質量分析装置に関するも
のである。
[Detailed description of the invention] The present invention relates to a mass spectrometer equipped with an electromagnetic device that generates a magnetic field for analysis, and in particular to a mass spectrometer that can eliminate relatively high-frequency magnetic field fluctuations caused by external magnetic lines of force coming from the outside. It is related to.

質量分析装置の分析用磁場は、装置が高分解能
になるほど強度変動が小さいことが望まれる。そ
こで、従来から磁場内にホール素子等の磁場強度
検出素子を配置し、該素子からの検出信号を基準
信号と比較し、その差が零になるように励磁電流
を制御し、磁場強度が常に一定になるようにして
いる。
The analytical magnetic field of a mass spectrometer is desired to have smaller intensity fluctuations as the resolution of the device increases. Therefore, conventionally, a magnetic field strength detection element such as a Hall element is placed in the magnetic field, the detection signal from the element is compared with a reference signal, and the excitation current is controlled so that the difference becomes zero, so that the magnetic field strength is always I try to keep it constant.

ところが、このような従来方法では、励磁コイ
ルのインダクタンスが大きいため、比較的ゆつく
りとした磁場変動を打消すことはできるものの、
例えば磁場を発生する電磁石のヨーク、励磁コイ
ル等に飛び込む外来磁力線による、分析磁場の比
較的周波数の高い(例えば数10Hz程度)微小な変
動を打消すことは困難であつた。
However, in such conventional methods, the inductance of the excitation coil is large, so although it is possible to cancel out the relatively slow fluctuations in the magnetic field,
For example, it has been difficult to cancel small fluctuations at a relatively high frequency (for example, on the order of several tens of Hz) in the analytical magnetic field caused by external magnetic lines of force that jump into the yoke of the electromagnet that generates the magnetic field, the excitation coil, etc.

本考案はこの点に鑑みてなさつれたものであ
り、イオンを質量電荷比に応じて分離するための
磁場を発生する電磁石装置と、該磁場の強度を掃
引するための手段とを備えた質量分析装置におい
て、上記電磁石装置の磁気回路中に配置される検
出コイルと、上記電磁石装置の磁気回路中に設置
される補助励磁コイルと、上記検出コイルからの
検出信号に基づいた電流を上記補助励磁コイルへ
供給するための電源と、該電源から補助励磁コイ
ルへ供給される電流を制限する電流制限回路とを
設けることにより、分析磁場の比較的周波数の高
い磁場変動を打消すことのできる質量分析装置を
提供することを目的としている。以下、図面を用
いて本考案を詳述する。
The present invention has been made in view of this point, and is a mass-mass device equipped with an electromagnetic device that generates a magnetic field for separating ions according to their mass-to-charge ratio, and a means for sweeping the strength of the magnetic field. In the analyzer, a detection coil disposed in the magnetic circuit of the electromagnet device, an auxiliary excitation coil disposed in the magnetic circuit of the electromagnet device, and a current based on the detection signal from the detection coil for the auxiliary excitation. Mass spectrometry that can cancel relatively high-frequency magnetic field fluctuations in the analytical magnetic field by providing a power supply for supplying the coil and a current limiting circuit that limits the current supplied from the power supply to the auxiliary excitation coil. The purpose is to provide equipment. Hereinafter, the present invention will be explained in detail using the drawings.

図面は、本考案の一実施例を示す構成図であ
る。図において、1はヨーク、2,3はポールピ
ース、4,5は励磁コイル、6は磁場制御電源で
ある。ポールピース2,3間に形成される磁場内
には、ホール素子等の磁場強度検出素子7が配置
され、該素子7から得られる検出信号は増幅器8
を介して前記磁場制御電源6へ送られる。該制御
電源6は検出信号と基準信号Rとの差信号に基づ
いて励磁コイル4,5へ供給する励磁電流を制御
するため、磁場強度は基準信号に対応する一定値
に保持されることになる。
The drawing is a configuration diagram showing an embodiment of the present invention. In the figure, 1 is a yoke, 2 and 3 are pole pieces, 4 and 5 are excitation coils, and 6 is a magnetic field control power source. A magnetic field strength detection element 7 such as a Hall element is arranged in the magnetic field formed between the pole pieces 2 and 3, and a detection signal obtained from the element 7 is sent to an amplifier 8.
The signal is sent to the magnetic field control power source 6 via the magnetic field control power source 6. Since the control power source 6 controls the excitation current supplied to the excitation coils 4 and 5 based on the difference signal between the detection signal and the reference signal R, the magnetic field strength is maintained at a constant value corresponding to the reference signal. .

このような制御系では周波数の高い外来磁力線
に起因する磁場変動を打消すことができないこと
は、先に述べた通りである。そこで、本考案にお
いては以下のような構成を付加している。即ち、
9は分析磁場を発生する電磁石の磁気回路中に配
置され、比較的周波数の高い磁場変動を検出する
検出コイル、10は磁場変動を打消す磁場を発生
する補助励磁コイルで、ヨーク1に直接巻かれて
おり、周波数特性を良くするため、該コイル10
のインダクタンスは例えば1mH以下にされてい
る。上記検出コイル9から得られた検出信号は、
増幅器11及び移相回路12を介して上記補助励
磁コイルへ電流を供給する電源13へ送られる。
該電源13と検出コイル9との間には、電流制限
回路14が挿入されている。
As mentioned above, such a control system cannot cancel magnetic field fluctuations caused by high-frequency external magnetic lines of force. Therefore, in the present invention, the following configuration is added. That is,
9 is a detection coil that is placed in the magnetic circuit of the electromagnet that generates the analysis magnetic field and detects relatively high-frequency magnetic field fluctuations; 10 is an auxiliary excitation coil that generates a magnetic field that cancels out the magnetic field fluctuations, and is wound directly on the yoke 1; In order to improve the frequency characteristics, the coil 10
For example, the inductance is set to 1 mH or less. The detection signal obtained from the detection coil 9 is
It is sent via an amplifier 11 and a phase shift circuit 12 to a power source 13 that supplies current to the auxiliary excitation coil.
A current limiting circuit 14 is inserted between the power source 13 and the detection coil 9.

かかる構成において、周波数の高い外乱磁束変
化は検出コイル9で電圧として検出され、得られ
た検出信号は移相回路12を介して移相が調整さ
れたのち、電源13へ送られる。該電源13は、
検出信号に応じた電流を補助励磁コイル10へ送
るが、該補助励磁コイルは検出された外乱磁場変
化を打消す方向の磁束を発生するような方向に巻
回されているため、外乱磁場は打消され、磁場は
高い周波数の変動に対しても安定化されることに
なる。
In this configuration, a high-frequency disturbance magnetic flux change is detected as a voltage by the detection coil 9, and the obtained detection signal is sent to the power source 13 after the phase shift is adjusted via the phase shift circuit 12. The power source 13 is
A current corresponding to the detection signal is sent to the auxiliary excitation coil 10, but since the auxiliary excitation coil is wound in a direction that generates magnetic flux in a direction that cancels out the detected disturbance magnetic field change, the disturbance magnetic field is canceled. The magnetic field will be stabilized even against high frequency fluctuations.

上記は磁場が定常状態にある場合であるが、質
量分析スペクトルを取得するために、基準信号R
を例えば鋸歯状波的に掃引する場合、検出コイル
9に磁場変化に基づく過大電圧が発生し、この過
大検出信号に基づき電源13は過大電流を補助励
磁コイル10へ流そうとするが、電流制限回路1
4により適宜な電流に制限されるため、磁場は掃
引中にあつても不安定にならない。
The above is a case where the magnetic field is in a steady state, but in order to obtain a mass spectrometry spectrum, the reference signal R
For example, when sweeping in a sawtooth waveform, an excessive voltage is generated in the detection coil 9 due to changes in the magnetic field, and based on this excessive detection signal, the power supply 13 attempts to flow an excessive current to the auxiliary excitation coil 10, but the current limit circuit 1
4, the magnetic field does not become unstable even during sweeping.

以上詳述した如く本考案によれば、定常状態に
おいても又掃引状態においても、磁場強度を高い
周波数の変動に対して安定化することのできる装
置が実現される。
As described in detail above, according to the present invention, an apparatus is realized that can stabilize the magnetic field strength against high frequency fluctuations both in a steady state and in a sweep state.

尚、上記実施例では電源13と補助励磁コイル
10の間に電流制限回路14を設けたが、増幅器
11と電源13との間に電圧制限回路を挿入して
も補助励磁コイル10へ供給される電流を制限す
ることが可能であり、更には、増幅器11に電圧
制限機能を持たせるようにしても良い。
In the above embodiment, the current limiting circuit 14 is provided between the power source 13 and the auxiliary excitation coil 10, but even if a voltage limiting circuit is inserted between the amplifier 11 and the power source 13, the current is still supplied to the auxiliary excitation coil 10. It is possible to limit the current, and furthermore, the amplifier 11 may have a voltage limiting function.

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

添付図面は本考案の一実施例を示す構成図であ
る。 1:ヨーク、2,3:ポールピース、9:検出
コイル、10:補助励磁コイル、12:移相回
路、13:電源、14:電流制限回路。
The accompanying drawings are block diagrams showing one embodiment of the present invention. 1: Yoke, 2, 3: Pole piece, 9: Detection coil, 10: Auxiliary excitation coil, 12: Phase shift circuit, 13: Power supply, 14: Current limiting circuit.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] イオンを質量電荷比に応じて分離するための磁
場を発生する電磁石装置と、該磁場の強度を掃引
するための手段とを備えた質量分析装置におい
て、上記電磁石装置の磁気回路中に配置される検
出コイルと、上記電磁石装置の磁気回路中に設置
される補助励磁コイルと、上記検出コイルからの
検出信号に基づいた電流を上記補助励磁コイルへ
供給するための電源と、該電源から補助励磁コイ
ルへ供給される電流を制限する電流制限回路とを
設けたことを特徴とする質量分析装置。
In a mass spectrometer equipped with an electromagnetic device that generates a magnetic field for separating ions according to their mass-to-charge ratio, and means for sweeping the intensity of the magnetic field, the method is arranged in a magnetic circuit of the electromagnetic device. a detection coil, an auxiliary excitation coil installed in the magnetic circuit of the electromagnet device, a power source for supplying a current to the auxiliary excitation coil based on a detection signal from the detection coil, and an auxiliary excitation coil from the power source. A mass spectrometer comprising: a current limiting circuit that limits the current supplied to the mass spectrometer.
JP747284U 1984-01-23 1984-01-23 mass spectrometer Granted JPS60121253U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP747284U JPS60121253U (en) 1984-01-23 1984-01-23 mass spectrometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP747284U JPS60121253U (en) 1984-01-23 1984-01-23 mass spectrometer

Publications (2)

Publication Number Publication Date
JPS60121253U JPS60121253U (en) 1985-08-15
JPH0342617Y2 true JPH0342617Y2 (en) 1991-09-06

Family

ID=30485856

Family Applications (1)

Application Number Title Priority Date Filing Date
JP747284U Granted JPS60121253U (en) 1984-01-23 1984-01-23 mass spectrometer

Country Status (1)

Country Link
JP (1) JPS60121253U (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS573360A (en) * 1980-06-06 1982-01-08 Jeol Ltd Mass spectroscope

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS573360A (en) * 1980-06-06 1982-01-08 Jeol Ltd Mass spectroscope

Also Published As

Publication number Publication date
JPS60121253U (en) 1985-08-15

Similar Documents

Publication Publication Date Title
US5517104A (en) Lead wire DC current sensor with saturated detecting core
JPS63301507A (en) Apparatus for compensating field interference varied with time in magnetic field
JPH0627151A (en) Amperometric converter operated on basis of compensation primciple
JPH07110085B2 (en) Magnetic adjuster for a long status magnetic levitation vehicle
JPH0342617Y2 (en)
US4972146A (en) Saturble core device with DC component elimination for measuring an external magnetic field
Huber et al. On the design of wide range electromagnets of high homogeneity
JP2752136B2 (en) Magnetic field generator
EP0278635B1 (en) Negative feedback power supply apparatus
EP0565177B1 (en) Device for determining the orientation of a vehicle
JPS6455023A (en) Rotary machine
SU1081498A1 (en) Electric magnet field stabilizer
JPH02229410A (en) Detection of direct-current deflecting magnetism in iron core of transformer
JPS5828708B2 (en) mass spectrometer
SU1038850A1 (en) Electron paramagnetic resonance radiospectrometer resonance condition stabilization method
JPH02117060A (en) Microbeam generator
JP3269437B2 (en) Ion synchrotron
JPS637419B2 (en)
SU653603A1 (en) Dc stabilizer
JPH08130803A (en) Vehicle
SU1554044A1 (en) Method of checking armature travel of electromagnetic switching apparatus
JPH0626804A (en) Method for exciting gap sensor
Marks Magnetic design of trim excitations for the Advanced Light Source storage ring sextupole
JPH0750597B2 (en) Quadrupole mass spectrometer
Fang et al. Analysis and measurements of eddy current effects of a beam tube in a pulsed magnet