Delay eliminating method for signal of self-powered vanadium detector based on H-infinity filtering
A self-sufficient detector and signal delay technology, applied in radiation measurement, neutron radiation measurement, instruments, etc., can solve problems such as difficult application
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[0073] Such as figure 1 The structural diagram of the vanadium self-sufficient neutron detector shown, in which the names of the components of each serial number correspond to: 1-emitter, 2-insulation layer, 3-collector, 4-wire, 5-protective shell, 6-insulation Cable, 7-current line, 8-base line, 9-sealed tube, 10-current output terminal. The characteristic parameters of the vanadium self-supplied neutron detector are: λ 1 =ln2 / 42.3s -1 =0.016386s -1 ,λ 2 =ln2 / 4.34 / 60s -1 =0.00266186s -1 , c=0.06, a 1 =0.879,a 2 = 0.061. image 3 It is a schematic diagram of the nuclear reaction between vanadium and neutrons, for image 3 During the reaction process, the figure 1 device for measurement. Such as figure 2 As shown, the method for eliminating the signal delay of vanadium self-powered detectors based on H∞ filtering includes the following steps in sequence: step 1, establishing the nuclear reaction model of vanadium and thermal neutrons; step 2, using direct transform...
Embodiment 2
[0112] This embodiment makes the following further limitations on the basis of Embodiment 1: in the case of shifting, it also includes processing the original signal according to the following signal processing method: in the shifting area, assuming that the neutron flux remain unchanged, then invert the current signal generated by the neutron flux density, and then subtract it from the actual output current of the detector to obtain the shift mutation component; outside the shift region, the detector output current minus the shift mutation component, The current signal generated by the neutron flux density is obtained, and then the delay elimination process is performed on the current signal.
[0113] The shift area design structure of the present embodiment is as follows:
[0114] In the shift area (k 1 ≤k≤k 2 ), assuming that the neutron flux density remains constant, then:
[0115] n(k+1)=n(k) (13)
[0116] J a (k+1)=e -λ·Ts J a (k)+(1-e -λ·Ts )n(k) (14)
[0117] ...
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