Signals Produced by Inconel Mineral Insulated Coaxial Cables in Neutron and Gamma-Ray Fields

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Signals Produced by Inconel Mineral Insulated Coaxial Cables in Neutron and Gamma-Ray Fields AECL-6876 ATOMIC ENERGY ^fflS L'ENERGIE ATOMIQUE OF CANADA LIMITED TiBV DU CANADA LIMITEE SIGNALS PRODUCED BY INCONEL MINERAL INSULATED COAXIAL CABLES IN NEUTRON AND GAMMA-RAY FIELDS Signaux produits par des cables coaxiaux a isolation minerale en Inconel dans des champs de neutrons et de rayons gamma C.J. ALLAN and G.F. LYNCH Chaik River Nuclear Laboratories Laboratoires nucle'aires de Chalk River Chalk River, Ontario July 1980 juillet ATOMIC ENERGY OF CANADA LIMITED SIGNALS PROVUCEV BV INCONEL MINERAL INSULATED COAXIAL CABLES IN NEUTRON ANP GAMMA-RAV FIELPS by C.J. Allan and G.F. Lynch Chalk River Nuclear Laboratories Chalk River, Ontario KOJ 1J0 1980 JU1^ AECL-6876 L'ÉNERGIE ATOMIQUE DU CANADA, LIMITÉE Signaux produits par des câbles coaxlaux â isolation minérale en Inconel dans des champs de neutrons et de rayons gamma par C.J. Allan et G.F. Lynch RÉSUMÉ Les câbles à isolation minérale, employés de concert avec des détecteurs de flux auto-alimentés dans les réacteurs CANDU, ont leur gaine et leur fil de noyau faits en Inconel 600 et leur isolation faite en MgO. On a entrepris une étude pour mieux connaître fondamentalement les processus produisant du courant dans les câbles à isolation minérale et pour déterminer dans quelle mesure ces processus sont apparentés aux geometries des câbles. Un certain nombre de câbles en Inconel-Inconel ont été irradiés dans le NRU, le ZED-2 et les réacteurs piscines d'essai à Chalk River ainsi que dans un irradiateur Gammacell-200 au cobalt-60. D'autres données ont été obtenues dans la centrale nucléaire Bruce A. Laboratoires nucléaires de Chalk River Chalk River, Ontario KOJ 1J0 Juillet 1980 AECL-6876 ATOMIC ENERGY OF CANADA LIMITED SIGNALS PROVUCEV BY INC0NEL MINERAL INSULATED COAXIAL CABLES IN NEUTRON ANP GAMMA-RA/ FIELDS by C.J. Allan and G.F. Lynch ABSTRACT Mineral insulated (MI) cables used with self-powered flux detectors in CANDU reactors employ Inconel 600 as the sheath and core-wire material, and MgO as the insulation. A study was undertaken to obtain a more fundamental understanding of the current producing processes in such MI cables and to determine how these processes are related to cable geometries. A number of Inconel-Inconel cables were irradiated in the NRU, ZED-2, and Pool Test reactors at CRNL and a Gammacell-220 6°Co irradiator. Additional data were obtained from the Bruce Nuclear Generating Station-A. Chalk River Nuclear Laboratories Chalk River, Ontario KOJ 1J0 1980 July AECL-6876 TABLE OF CONTENTS Page LIST OF FIGURES [II) LIST OF TABLES \lv) 1. INTRODUCTION 1 1.1 The Use of Mineral Insulated Cables in 1 Reactors 1.2 The Interaction of Reactor Radiation with 2 Cables 1.3 Cable Geometries Studied 5 2. EXPERIMENTAL STUDIES 5 2.1 Gamma-Ray Studies 5 2.1.1 Gammacell Tests 5 2.1.2 Reactor Gamma Rays 12 2.1.3 Conclusion on y~RaY Sensitivity 17 2.2 NRU Irradiations 18 2.2.1 Introduction 18 2.2.2 Variation of Signal with Core 21 Penetration 2.2.3 Variation of Sensitivity with 24 Core-Wire Diameter 2.2.4 Conclusions 34 2.3 Irradiations in the Pool Test Reactor 35 2.4 ZED-2 Tests 38 2.5 Results Obtained from Bruce NGS-A 43 2.5.2 Results from Unit 3 43 2.5.3 Summary . 55 3. SUMMARY AND CONCLUSIONS 56 4. ACKNOWLEDGEMENTS 58 5. REFERENCES 58 \U] LIST OF FIGURES FIGURE 1 Variation of the y-ray Sensitivities for Lead Cables SC-601 to SC-606 with Sheath Mass FIGURE 2 Variation of the yray Sensitivities for 11 Lead Cables VC-501 to VC-505 and TC-101 to TC-105 with Sheath Mass FIGURE 3 Schematic of the Test Section of the X-6 14 Test Loop in the NRX Reactor. The Detectors are Designated RV for Vanadium, RP for Platinum and RC for Cobalt. In Total, some 14 Detectors are Mounted Along the Length of the Pressure Tube. Only the 6 Detectors Contained Within the 3He Coil Are Shown Here. FIGURE 4 Cross Section of the NRU Test Assembly in 19 Which the Lead Cables Were Irradiated FIGURE 5 The Current Generated in the Miniature 20 Fission Chamber Used to Measure the Lead Cable Sensitivity as a Function of TFD Position FIGURE 6 Variation of the Total Sensitivities of 26 the IMI Cable with Core-Wire Diameter FIGURE 7 Variation of the (n,g) Sensitivity, 28 S(n,$) with Core-Wire Diameter FIGURE 8 The Variation of the So-Called Reduced 30 Sensitivity, SR, with Core-Wire Diameter FIGURE 9 Variation of the (n,Y,e) Sensitivity 32 with Core-Wire Diameter for the IMI Cables Irradiated in NRU FIGURE 10 The Currents Generated in Lead Cables 36 TC-101 to TC-105 and VC-501 to VC-505, as a Function of Core-Wire Diameter, for an Irradiation in the Pool Test Reactor LIST OF FIGURES (continued) Page FIGURE 11 The Current Generated in Lead Cables 39 TC-101 to TC-105, as a Function of Core-Wire Diameter, for an Irradiation in the ZED-2 Reactor FIGURE 12 Schematic Representation of the ZED-2 40 Reactor Showing the Location of the Test Rod Relative to the Fuel Assemblies FIGURE 13 Schematic Representation of the Test 4 2 Assembly Used for Irradiating Lead Cables UC-103 to UC-106 in the ZED-2 Reactor FIGURE 14 Schematic Representation of the Bruce 44 NGS-A Reactor Showing the Location of Flux Detector Assemblies NFM-1 to NFM-20 FIGURE 15 Schematic Representation of Flux Detector 4 5 Rod, NFM-1, Installed in the Bruce NGS-A, Unit 1 Reactor FIGURE 16 Relative Sensitivities of Lead Cables 4 6 TC-101 to TC-105, as a Function of Core-Wire Diameter, Determined in the Bruce NGS-A, Unit 1 Reactor FIGURE 17 The Signal for a Test Lead Cable, 50 Installed in the Bruce NGS-A, Unit 3 Reactor, as a Function of Time, Following the Reactor Trip. The Results were Obtained During Phase B Commissioning of the Reactor FIGURE 18 Relative Sensitivity for the 1.0 mm 53 O.D. Lead Cables Installed in the Bruce NGS-A, Unit 3 Reactor as a Function of Core-Wire Diameter FIGURE 19 The Flux Distribution Along Flux 54 Detector Rod NFM-6, Bruce NGS-A, Unit 3, Determined During Phase B Commissioning of the Reactor LIST OF TABLES Page TABLE 1 Description of Experimental Cables 6 TABLE 2 Summary of the Dimensions of the Lead Cables 8 Irradiated in the Gammacell-220 Irradiator and the y~RaY Sensitivities Determined in These Irradiations TABLE 3 Summary of the Lengths and the Experimental 23 Results Obtained with the Lead Cables Which Penetrated the NRU Core to Different Elevations TABLE 4 Summary of the Dimensions and the 25 Sensitivities of the IMI Lead Cables Irradiated in the NRU Reactor TABLE 5 Summary of the Sensitivities Determined for 41 Lead Cables UC-103 to UC-106 in the ZED-2 Reactor and NRU Reactor TABLE 6 Summary of the Currents from the Lead 48 Cables Installed in the Bruce NGS-A, Unit 3 Reactor as a Function of Time During Phase B Testing. The Reactor was Raised to 10~2 of Full Power at t=0 and Tripped at t=327 min. These Data Have Been Used to Estimate the Current Due to the Decay of 5eMn and 65Ni, I,(n,B), as Discussed in the Text. TABLE 7 Summary of the Results Obtained from 49 the 1.0 mm and L6 mm IMI Lead Cables Installed in the Bruce NGS-A, Unit 3 Reactor TABLE 8 Summary of the Currents Generated by 55 1.0 mm O.D. Lead Cables of Different Lengths, for the Nominal Bruce Core, as a Function of Time After Reaching 10~2 Full Power. The Lengths of the Lead Cables are Shown in Figure 16. SIGNALS PROVUCEV BV INCOMEL MINERAL INSULATEP COAXIAL CABLES IN NEUTRON ANP GAMMA-RA/ FIELPS by C.J. Allan and G.F. Lynch 1. INTRODUCTION 1.1 The Use of Mineral Insulated Cables in Reactors Because self-powered detectors (SPDs) are relatively simple, rugged, and cheap to manufacture, they are used exten- sively in CANDU nuclear reactors to (i) provide information on the distribution of flux throughout the core [1], (ii) for bulk and spatial control of the reactor [2], and (iii) for overpower protection. In most applications, a SPD consists of a coaxial cable having a metallic outer sheath, frequently the Ni-Cr-Fe alloy Inconel 600; a mineral oxide insulation layer, usually MgO or Al_O,; and a metallic central wire, commonly called the emitter. When such a device is placed in a radiation field, as for example in the neutron field in the core of a nuclear reactor and the central conductor is connected to the sheath through an ammeter, a current flows between the two electrodes without an external bias being applied. The magnitude of the current is proportional to the intensity of the radiation field, and hence can be used as a measure of the field strength. In most reactor applications, a SPD is used to measure the average flux over a localized region of the core and a lead cable must be used to bring the current signal from the detector to the measurement instrumentation. In CANDU reactors, the lead - 2 - cable is a mineral insulated (MI) coaxial cable, 1.0 mm O.D., with reactor-grade Inconel 600 being used for the sheath and core wire, and compacted MgO being used as the insulant.
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