Delay eliminating method for signal of self-powered rhodium detector based on H2/H-infinity hybrid filtering
A technology of self-powered detectors and signal delays, applied in radiation measurement, neutron radiation measurement, instruments, etc., can solve problems that are difficult to apply and obtain statistical characteristics
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[0077] Such as figure 1 The structure diagram of rhodium self-sufficient neutron detector shown, in which the names of the parts 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 parameter of this rhodium self-supplied energy neutron detector is: 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 the principle process diagram of rhodium and neutron nuclear reaction, for image 3 During the reaction process, the figure 1 device for measurement. Such as figure 2 As shown, the rhodium self-powered detector signal delay elimination method based on H2 / H∞ hybrid filtering includes the following steps in sequence: step 1, establish the nuclear reaction model of rhodium and thermal neutrons; step 2, use direct transformation to establish ...
Embodiment 2
[0123] This embodiment makes the following further limitations on the basis of Embodiment 1: In the case of shifting, this embodiment also includes processing the original signal according to the following signal processing method: in the shifting area, assuming The sub-flux remains unchanged, and then the current signal generated by the neutron flux density is reversed, and then subtracted from the actual output current of the detector to obtain the shifting mutation component; outside the shifting area, the detector output current minus the shifting The mutation component is obtained to obtain the current signal generated by the neutron flux density, and then the delay elimination process is performed on this current signal.
[0124] The shift area design structure of the present embodiment is as follows: in the shift area (k 1 ≤k≤k 2 ), assuming that the neutron flux density remains constant, then:
[0125] n(k+1)=n(k) (15)
[0126] J a ...
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