H<infinity> filtration-based signal delay elimination method for rhodium self-powered detector
A self-sufficient energy detector and signal delay technology, applied in the fields of instrumentation, informatics, nuclear power generation, etc., can solve problems that are difficult to apply
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[0090] like 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 rhodium self-supplied energy neutron detector, its characteristic parameter 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. like figure 2 As shown, the method for eliminating the signal delay of rhodium self-powered detectors based on H∞ filtering includes the following steps carried out in sequence: Step 1, establishing the nuclear reaction model of rhodium and thermal neutrons; Step 2, adopting decoupling transformat...
Embodiment 2
[0145] 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.
[0146] The shift area design structure of the present embodiment is as follows:
[0147] In the shift area (k 1 ≤k≤k 2 ), assuming that the neutron flux density remains constant, then:
[0148] n(k+1)=n(k) (19)
[0149] x ...
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