JPS6464639A - Nuclear magnetic resonance imaging apparatus - Google Patents
Nuclear magnetic resonance imaging apparatusInfo
- Publication number
- JPS6464639A JPS6464639A JP62221925A JP22192587A JPS6464639A JP S6464639 A JPS6464639 A JP S6464639A JP 62221925 A JP62221925 A JP 62221925A JP 22192587 A JP22192587 A JP 22192587A JP S6464639 A JPS6464639 A JP S6464639A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- memory element
- inclined magnetic
- current waveform
- intensity
- 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.)
- Pending
Links
- 238000013421 nuclear magnetic resonance imaging Methods 0.000 title 1
- 230000000630 rising effect Effects 0.000 abstract 2
- 238000003384 imaging method Methods 0.000 abstract 1
- 238000005259 measurement Methods 0.000 abstract 1
Landscapes
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
PURPOSE:To obtain an inclined magnetic field always having a definite rising/falling time and flatness, by preliminarily storing the optimum current waveform at each intensity of an inclined magnetic field in a memory element and using the corresponding data on the memory element at the time of imaging. CONSTITUTION:A memory element 26 for storing a current waveform is arranged to the pre-stage of a DAC (D/A converter) 21 and the optimum current waveform corresponding to the intensity of each inclined magnetic field is preliminarily stored in said memory element. When a current is allowed to flow to an inclined magnetic field coil, the data of the current waveform corresponding to a necessary inclined magnetic field is drawn out by the order from a sequencer. The data of the memory element is converted to an analogue signal by the DAC while said analogue signal is sent to an amplifier as it is to be applied to the inclined magnetic field coil of load. By this circuit constitution, the optimum current waveform is already obtained in the stage of the memory element and, therefore, it is unnecessary to shape a signal waveform after the DAC. When all of the current waveforms corresponding to the intensity of the inclined magnetic fields necessary for actual measurement are stored in the memory element, an inclined magnetic field having a definite rising/falling time and flatness is obtained without relying on intensity.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62221925A JPS6464639A (en) | 1987-09-07 | 1987-09-07 | Nuclear magnetic resonance imaging apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62221925A JPS6464639A (en) | 1987-09-07 | 1987-09-07 | Nuclear magnetic resonance imaging apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6464639A true JPS6464639A (en) | 1989-03-10 |
Family
ID=16774306
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62221925A Pending JPS6464639A (en) | 1987-09-07 | 1987-09-07 | Nuclear magnetic resonance imaging apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6464639A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014045775A (en) * | 2012-08-29 | 2014-03-17 | Toshiba Corp | Magnetic resonance imaging apparatus |
-
1987
- 1987-09-07 JP JP62221925A patent/JPS6464639A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014045775A (en) * | 2012-08-29 | 2014-03-17 | Toshiba Corp | Magnetic resonance imaging apparatus |
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