NEUTRON MEASUREMENT APPARATUS AND NEUTRON MEASUREMENT METHOD

• US 20130221231A1
• Filed: 02/28/2013
• Published: 08/29/2013
• Est. Priority Date: 02/29/2012
• Status: Active Grant

• Current Assignee: Kabushiki Kaisha Toshiba (Toshiba Corporation)
• Original Assignee: Kabushiki Kaisha Toshiba (Toshiba Corporation)
• Inventors: KONO, Shigehiro, Tomitaka, Makoto
• Granted Patent: US 8,878,139 B2
• Time in Patent Office: Days
• US Class Current: 250/391
• CPC Class Codes: G01T 1/17 Circuit arrangements not adapted to a particular type of detector pulse-selection circuits H03K, G01R
• CPC Class Codes: G01T 3/00 Measuring neutron radiation G01T5/00 takes precedence

Abstract

A neutron measurement apparatus includes: an analog signal processor; a digitizing processor; an FFT calculation processor; and a signal processor. The analog signal processor amplifies alternating current components of detector output signals output from a neutron detector, and filters to remove high frequency components from the output signals, which the digitizing processor digitizes at a constant sampling period in a time series; the FFT calculation processor converts certain of the signals in a time domain from the digitizing processor into signals in a frequency domain, and filters the signals in the frequency domain; and the signal processor selects and extracts signals having required frequency components through the calculation processing on the FFT calculation processor, to calculate power spectral densities of the extracted signals, and to convert the calculated power spectral densities into a neutron measurement value.

Claims

1. A neutron measurement apparatus comprising:

an analogue signal processing system configured to amplify alternating current components of detector output signals output from a neutron detector, and to apply filtering to remove high frequency components from the output signals;

a digitizing processing system configured to digitize the output signals output from the analogue signal processing system at a constant sampling period in a time series;

a FFT calculation processing system configured to convert a certain number of the signals in a time domain output from the digitizing processing system into signals in a frequency domain, and to apply filtering to the signals in the frequency domain; and

a signal processing system configured to select and extract signals having required frequency components through the calculation processing on the FFT calculation processing system, so as to calculate power spectral densities of the extracted signals, and to convert the calculated power spectral densities into a neutron measurement value.

2. The neutron measurement apparatus according to claim 1, wherein

the FFT calculation processing system includes an FFT device configured to apply fast Fourier transform processing to the signals in the time domain output from the digitizing processing system, so as to convert the signals in the time domain into the signals in the frequency domain.

3. The neutron measurement apparatus according to claim 1, wherein

the signal processing system includes:

a signal selecting device configured to select and extract the signals having required frequency components based on a calculation result of the FFT calculating processing system;

a power spectral density calculator configured to calculate the power spectral densities of the signals selected and extracted on the signal selecting device; and

a neutron signal converter configured to convert the power spectral densities into a neutron measurement value.

9. The neutron measurement apparatus according to claim 1, wherein

the signal processing system includes an accuracy-or-responsivity selecting unit having a function of selecting a standard deviation or responsivity of a neutron measurement result, and

the signal processing system has a function to apply a weighted mean calculation on a weighted mean calculator to plural power spectral densities calculated on the power spectral density calculator based on the selected standard deviation or responsivity, or to plural neutron measurement values output from the neutron signal converter.

11. The neutron measurement apparatus according to claim 1, wherein

the signal processing system:

includes all or a part of constituent elements of claim 5 to claim 10;

has a function of selecting at least one of parameters including a resampling period, a degree of the FFT, a number of the power spectral densities or of the neutron measurement values to be subjected to the weighted mean calculation, and a standard deviation or responsivity of a neutron measurement result; and

has a function of setting unselectable parameters to be fixed or automatically selectable, and displaying parameters automatically selected.

4. A neutron measurement apparatus comprising:

a preamplifier configured to amplify detector output signals from a neutron detector ;

an AC amplifier configured to amplify alternating current components of the signals output from the preamplifier;

an analogue filter device configured to remove high frequency components from the signals output from the AC amplifier;

an AD converter configured to AD-convert the output signals from the analogue filter device at a constant sampling period into digital signals;

a recorder configured to record the digital signals converted on the AD converter;

a window function multiplier configured to read out a certain number of the digital signals from the recorder, and to multiply the digital signals by window function coefficients;

an FFT device configured to apply fast Fourier transform processing to the output signals from the window function multiplier;

a signal selecting device configured to select and extract only signals having required frequency components based on a calculation result of the FFT device;

a power spectral density calculator configured to calculate power spectral densities of the signals selected and extracted on the signal selecting device; and

a neutron signal converter configured to convert the output signals from the power spectral density calculator into a neutron measurement value.

5. The neutron measurement apparatus according to claim 4, wherein

a frequency range selected by the signal selecting device is set to be variable, and

the neutron signal convertor performs correction depending on the selected frequency range.

6. The neutron measurement apparatus according to claim 5, wherein

if such FFT-processed signals are removed that correspond to a frequency band including part of a frequency response characteristic range of any measurement system from the neutron detector before the signals are converted into the digital signals,

the neutron signal converter performs correction corresponding to the part of frequency response characteristic of the measurement system included in the removed frequency band.

7. The neutron measurement apparatus according to claim 4, wherein

the neutron measurement apparatus includes a lowpass filter, and a down-sampling device for decreasing a sampling period in a step subsequent to the AD converter, so as to allow the sampling period to be variable, and also allow a selecting range of the FFT-processed signals in the frequency domain to be changeable, wherein the selecting range is selected on the signal selecting device depending on the sampling period.

8. The neutron measurement apparatus according to claim 4, wherein

the FFT device is configured to:

allow a number of digital signals to be fast Fourier transform (FFT)-processed to be variable;

allow a selecting range of the FFT-processed signals in the frequency domain to be changeable, wherein the selecting range is selected on the signal selecting device depending on the selected number of the digital signals; and

correct the neutron measurement value on the neutron signal converter depending on the FFT-processed signals in the frequency domain selected on the signal selecting device.

10. The neutron measurement apparatus according to claim 4, wherein

the signal processing system includes an accuracy-or-responsivity selecting unit having a function of selecting a standard deviation or responsivity of a neutron measurement result, and

the signal processing system has a function to apply a weighted mean calculation on a weighted mean calculator to plural power spectral densities calculated on the power spectral density calculator based on the selected standard deviation or responsivity, or to plural neutron measurement values output from the neutron signal converter.

12. The neutron measurement apparatus according to claim 4, wherein

the signal processing system:

includes all or a part of constituent elements of claim 5 to claim 10;

has a function of selecting at least one of parameters including a resampling period, a degree of the FFT, a number of the power spectral densities or of the neutron measurement values to be subjected to the weighted mean calculation, and a standard deviation or responsivity of a neutron measurement result; and

has a function of setting unselectable parameters to be fixed or automatically selectable, and displaying parameters automatically selected.

13. A neutron measurement method comprising:

amplifying alternating current components of detector output signals output from a neutron detector, and applying filtering to the output signals to remove high frequency components from the output signals on an analogue signal processing system;

digitizing the processed detector output signals at a constant sampling period in a time series on a digitizing processing system;

applying fast Fourier transform (FFT) processing to the digitized signals in a time domain to convert the signals into signals in a frequency domain on an FFT calculation processing system, and applying filtering to the FFT-processed signals in the frequency domain; and

selecting and extracting signals having required frequency components from the FFT-processed signals in the frequency domain, so as to calculate power spectral densities of the extracted signals, and obtain a neutron measurement value based on the power spectral densities of the extracted signals.