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by JK Chakravartty and R. Kapoor Mechanical Metallurgy Division and AK Suri Materials Group PDF

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BARC/2011/E/017 B A R C /2 0 1 1 /E /0 1 7 THERMOMECHANICAL PROCESSING OF Nb-1Zr-0.1C ALLOY FOR USE IN COMPACT HIGH TEMPERATURE REACTORS: A FIRST REPORT by J.K. Chakravartty and R. Kapoor Mechanical Metallurgy Division and A.K. Suri Materials Group 2011 7 BARC/2011/E/017 1 0 / E / 1 1 0 2 / C GOVERNMENT OF INDIA R A ATOMIC ENERGY COMMISSION B THERMOMECHANICAL PROCESSING OF Nb-1Zr-0.1C ALLOY FOR USE IN COMPACT HIGH TEMPERATURE REACTORS: A FIRST REPORT by J.K. Chakravartty and R. Kapoor Mechanical Metallurgy Division and A.K. Suri Materials Group BHABHA ATOMIC RESEARCH CENTRE MUMBAI, INDIA 2011 BARC/2011/E/017 BIBLIOGRAPHIC DESCRIPTION SHEET FOR TECHNICAL REPORT (as per IS : 9400 - 1980) 01 Security classification : Unclassified 02 Distribution : External 03 Report status : New 04 Series : BARC External 05 Report type : Technical Report 06 Report No. : BARC/2011/E/017 07 Part No. or Volume No. : 08 Contract No. : 10 Title and subtitle : Thermomechanical processing of Nb-1Zr-0.1C alloy for use in compact high temperature reactors: a first report 11 Collation : 41 p., 12 figs., 3 tabs., 1 ill. 13 Project No. : 20 Personal author(s) : 1) J.K. Chakravartty; R. Kapoor 2 ) A.K. Suri 21 Affiliation of author(s) : 1) Mechanical Metallurgy Division, Bhabha Atomic Research Centre, Mumbai 2 ) Materials Group, Bhabha Atomic Research Centre, Mumbai 22 Corporate author(s) : Bhabha Atomic Research Centre, Mumbai - 400 085 23 Originating unit : Mechanical Metallurgy Division, BARC, Mumbai 24 Sponsor(s) Name : Department of Atomic Energy Type : Government Contd... i BARC/2011/E/017 30 Date of submission : July 2011 31 Publication/Issue date : August 2011 40 Publisher/Distributor : Head, Scientific Information Resource Division, Bhabha Atomic Research Centre, Mumbai 42 Form of distribution : Hard copy 50 Language of text : English 51 Language of summary : English, Hindi 52 No. of references : 33 refs. 53 Gives data on : 60 Abstract : Nb-1Zr-0.1C is a potential material for use in high temperature nuclear reactors. Use of this alloy in components requires appropriate thermomechanical processing to break the cast microstructure and to obtain uniformly distributed fine stable precipitates so as to produce the desired mechanical properties at the high operating temperatures. This report reviews the thermomechanical processing of Nb-1Zr-0.1C alloy carried out over the years by other researchers and the high temperature creep behavior of the alloy. The hot deformation of Nb-1Zr-0.1C alloy carried out at Mechanical Metallurgy Division is also presented here. From this review it is evident that most primary hot working studies were carried out between 1500 to 1700 °C. The subsequent annealing treatments, which require holding at lower temperatures of about 1100 to 1300 °C for very long times help further transform the precipitates from coarse orthorhombic to very fine cubic. Our studies on Nb-1Zr-0.1C alloy also confirm that optimum hot working lies at temperatures beyond 1500 °C where dynamic recrystallization initiates, and optimally around 1700 °C where dynamic recrystallization transforms the microstructure. Working at temperatures lower than 1000 °C may lead to the undesirable effect of both micro as well as macro strain localization, and should be avoided. 70 Keywords/Descriptors: NIOBIUM ALLOYS; ZIRCONIUM ALLOYS; CASTING; MICROSTRUCTURE; RECRYSTALLIZATION; CREEP; YIELD STRENTH; EMBRITTLEMENT; GRAIN BOUNDARIES 71 INIS Subject Category : S 36 99 Supplementary elements : ii Table of Contents List of Figures iv List of Tables v Abstract 1 1 Introduction 2 2 Precipitates in Nb alloys 7 3 Processing of cast ingots 10 4 Creep of Nb-1Zr alloys 14 5 Summary 19 6 Recommendations for hot working of Nb-1Zr-0.1C 20 Reference 22 Annexure I - Work carried out at MMD, BARC, compiled as paper 23       iii List of Figures Fig. 1. Comparison of yield stress of some refractory alloys. T-111: Ta-8.7W-0.04Zr; TZM: Mo-0.5Ti-0.1Zr; C103: Nb-10Hf-1Ti-0.5Zr; PWC-11: Nb-1Zr-0.1C from [5], and Nb-5W-2Mo-1Zr from [6]. 3 Fig. 2. Comparison of the UTS of some refractory alloys. Adapted from [7]. 3 Fig. 3. Recommended stress – temperature design domain of Nb-1Zr based on radiation embrittlement, recrystallization, creep and the ultimate tensile strength [5]. 5 Fig. 4. Operating temperature window for V, Nb, Ta, Mo and W refractory alloys, Fe- 9%Cr ferritic-martensitic steel, Fe 13%Cr oxide dispersion strengthened ferritic steel, 316 austenitic stainless steel, solutionized and aged Cu–2%Ni– 0.3%Be, and SiC/SiC composites. The light shaded areas represent uncertainties in the minimum and maximum temperature limits [11]. 6 Fig. 5. Room temperature strength (YS and UTS) vs. ductility plot for different Nb alloys; data extracted from Ref. [10]. 7 Fig. 6. The ratio of Zr/Nb in precipitates plotted against time of aging at 1077 °C comparing two studies. Prior to aging the samples were double annealed at 1482 °C for 1 h followed by 1202 °C for 2 h. 9 Fig. 7. TEM micrograph and diffraction pattern of extracted carbide particles from Nb-1Zr-0.1C alloy after extrusion at 1600 °C, cold work of 90% followed by two part anneal of 1 h at 1482 °C + 2 h at 1204 °C [21]. 10 Fig. 8. Back scattered SEM image of Nb-1Zr annealed at 1560 °C and aged for 1100 h at (a) 975 °C and (b) 1125 °C showing Zr O precipitates both at grain 2 boundaries and within grains [23]. 10 Fig. 9. Creep rate vs. creep strain for Nb-1Zr and PWC-11 in different conditions, tested at 1077 °C and 40 MPa. The annealed condition for Nb-1Zr is 1482 °C for 1 h. The annealed condition for PWC-11 is 1482 °C for 1 h followed by 1202 °C for 2 h. Two aging conditions after annealing for PWC-11 are shown: aging at 1077 °C for 1000 h and 1127 °C for 1000 h. Data taken from Titran [22]. 15 Fig. 10. Plot of pseudo strain rate vs. test stress for Nb alloys in different conditions. Nb-1Zr was annealed at 1202 °C for 1 h. PWC-11 was annealed at 1482 °C for 1 h followed by 1202 °C for 2 h, the aging condition was 1077 °C for 1000 h. C103 was annealed at 1337 °C for 1 h. Taken from from Refs. [22, 30]. 16 Fig. 11. Steady state strain rate vs. applied stress for pure Nb, Nb-1Zr, and Nb-1Zr- 0.1C at 1027 °C (taken from [21]). The stress exponent for all of them is about 6. 17 Fig. 12. Comparison of the creep rate vs. strain plot for Nb-1Zr and PWC-11 taken from Titran [22, 29] and Nb-1Zr taken from [31]. For the sake of comparison the data of Davidson is converted to same stress and temperature as described in text. Note that the creep strain axis has a break from 0.02 to 0.3. 18 iv List of Tables Table 1: Commercially available Nb alloys for use at high temperatures [10]. 5 Table 2: Precipitation reaction in Nb-10W-1Zr-0.1C. M(ss) represents the solid solution, M’ is solid solution in metastable equilibrium with M C, and 2 M is solid solution in equilibrium with monocarbide MC [14]. 8 Table 3. Summary of the hot working conditions to break the cast microstructure of Zr-1Nb-0.1C of the materials used by researchers. The source of the material is written in brackets. 13 v ÃÖÓÆüŸÖ ˆ““Ö ŸÖÖ¯Ö´ÖÖ−Ö ×¸ü‹Œ™ü¸üÖë ´Öë ¯ÖÏμÖÖêÖ ÆêüŸÖã Nb-1Zr-0.1C ×´ÖÁÖ¬ÖÖŸÖ㠍úÖ ŸÖÖ¯ÖμÖÖÓס֍ú ÃÖÓÃÖÖ¬Ö−Ö : ¯ÖÏ£Ö´Ö ×¸ü¯ÖÖê™Ôü •Öê.êú. “֍Îú¾ÖŸÖá, †Ö¸ü. ú¯Öæ¸ü, ‹.êú.ÃÖæ¸üß μÖÖÓס֍ú ¬ÖÖŸÖãúß ¯ÖϳÖÖÖ ¯Ö¤üÖ£ÖÔ ¾ÖÖÔ, ³ÖÖ³ÖÖ ¯Ö¸ü´Ö֝Öã †−ÖãÃÖÓ¬ÖÖ−Ö ëú¦ü, ´ÖãÓ²Ö‡Ô ÃÖÖ¸üÖÓ¿Ö ˆ““Ö ŸÖÖ¯Ö´ÖÖ−Ö −ÖÖ׳֍úßμÖ ×¸ü‹Œ™ü¸üÖë ´Öë ¯ÖÏμÖÖêÖ ÆêüŸÖã Nb-1Zr-0.1C ‹ú ×¾Ö³Ö¾Ö ¯Ö¤üÖ£ÖÔ Æîü … ‡ÃÖ ×´ÖÁÖ ¬ÖÖŸÖ㠍úÖ ¯ÖÏμÖÖêÖ †Ö¾Ö¿μ֍ú ‘Ö™üúÖë ´Öë ÆüÖêŸÖÖ Æîü ‡Ã֍êú ×»Ö‹ †Ö¾Ö¿μ֍ú Æîü ׍ú ˆ×“ÖŸÖ ŸÖÖ¯ÖμÖÖÓס֍ú ÃÖÓÃÖÖ¬Ö−Ö «üÖ¸üÖ úÖÙü ´ÖÖ‡ÎúÖêÙÒêüŒ“Ö¸ü úÖê ŸÖÖê›ÍüÖ •ÖÖ‹ †Öî¸ü ‹ú ÃÖ´ÖÖ−Ö ×¾ÖŸÖ׸üŸÖ Ûãָü †¾ÖÖê¯ÖÖë úÖê ¯ÖÏÖ¯ŸÖ ú¸ü−Öê êú ×»Ö‹ ׍úμÖÖ •ÖÖ‹ ŸÖÖ׍ú ˆ““Ö ¯ÖÏ“ÖÖ»Ö−Ö ŸÖÖ¯Ö´ÖÖ−ÖÖë ¯Ö¸ü †¯Öê×ÖŸÖ μÖÖÓס֍ú ÖãÖ¬Ö´ÖÖí úÖ ˆŸ¯ÖÖ¤ü−Ö ×úμÖÖ •ÖÖ Ã֍êú … ‡ÃÖ ×¸ü¯ÖÖê™Ôü ´Öë †−μÖ †−ÖãÃÖÓ¬ÖÖ−֍úŸÖÖÔ†Öë «üÖ¸üÖ Nb-1Zr-0.1C ×´ÖÁÖ¬ÖÖŸÖ㠍êú ŸÖÖ¯ÖμÖÖÓס֍ú ÃÖÓÃÖÖ¬Ö−Ö ¯Ö¸ü †−Öêú ¾ÖÂÖÖí ÃÖê ׍ú‹ Ö‹ úÖμÖÖí †Öî¸ü ×´ÖÁÖ¬ÖÖŸÖ㠍êú ˆ““Ö ŸÖÖ¯Ö´ÖÖ−Ö ×¾ÖÃÖ¯ÖÔÖ †Ö“Ö¸üÖ úß ÃÖ´Ö߁ÖÖ úß Ö‡Ô Æîü … μÖÖÓס֍ú ¬ÖÖŸÖãúß ¯ÖϳÖÖÖ ´Öë Nb-1Zr-0.1C ×´ÖÁÖ¬ÖÖŸÖ㠍êú ŸÖ¯ŸÖ ×¾Öºþ¯ÖÖ ¯Ö¸ü ׍ú‹ Ö‹ úÖμÖÖí úÖê ³Öß ¯ÖÏßÖãŸÖ ׍úμÖÖ ÖμÖÖ Æîü … ‡ÃÖ ÃÖ´Ö߁ÖÖ ÃÖê ×ÃÖ¨ü ÆüÖêŸÖÖ Æîü ׍ú †×¬ÖúŸÖ¸ü ¯ÖÏÖ£Ö״֍ú ŸÖ¯ŸÖ 0 úÖμÖԍúÖ¸üß †¬μÖμÖ−Ö 1500 ÃÖê 1700 C êú ´Ö¬μÖ ×ú‹ Ö‹ Æïü … †−Öã¾ÖŸÖá ŸÖÖ¯ÖÖ−Öã¿ÖߟÖ−Ö ŸÖÖ¯Ö´ÖÖ−Ö, 0 וÖ−֍úß †Ö¾Ö¿μ֍úŸÖÖ ú¸üß²Ö 1100 ÃÖê 1300 C êú ×−Ö´−ÖŸÖ¸ü ŸÖÖ¯Ö´ÖÖ−ÖÖë úÖê »Ö´²Öê ÃÖ´ÖμÖ ŸÖú ²Ö−ÖÖ‹ ¸üÖ−Öê êú ×»Ö‹ ÆüÖêŸÖß Æîü, ˆ−Ö ÃÖê ¯Öã−Ö: †¾ÖÖê¯ÖÖë úÖê †¯Ö׸üéúŸÖ †Ö£ÖÖìÆüÖê´Ö׾֍ú ÃÖê ÁÖêšüŸÖ´Ö ‘Ö−Ö֍éú×ŸÖ ´Öë ¯Ö׸ü¾ÖÙŸÖŸÖ ú¸ü−Öê ´Öë ÃÖÆüÖμÖŸÖÖ ×´Ö»ÖŸÖß Æîü … Nb-1Zr-o.1C ×´ÖÁÖ¬ÖÖŸÖ ã ¯Ö¸ü Æü´ÖÖ¸êü †¬μÖμÖ−ÖÖë ÃÖê μÖÆü ³Öß 0 ×ÃÖ¨ü ÆüÖêŸÖÖ Æîü ׍ú ÃÖ¾ÖÖì¢Ö´Ö ŸÖ¯ŸÖ úÖμÖÔ 1500 C ÃÖê ¯Ö¸êü ŸÖÖ¯Ö´ÖÖ−ÖÖë ¯Ö¸ü ÆüÖêŸÖê Æîü •ÖÆüÖÓò Öן֍ú ¯Öã−Ö: 0 ׍ÎúÙü»Ö−Ö †Ö¸Óü³Ö ÆüÖêŸÖÖ Æîü †Öî¸ü ú¸üß²Ö 1700 C ¯Ö¸ü •ÖÆüÖÑ Öן֍ú ¯Öã−Ö: ׍ÎúÙü»Ö−Ö ´ÖÖ‡ÎúÖêÙÒêüŒ“Ö¸ü ´Öë 0 ¯Ö׸ü¾ÖÙŸÖŸÖ ÆüÖê •ÖÖŸÖÖ Æîü … 1000 C ÃÖê ú´Ö ¯Ö¸ü úÖμÖÔ ú¸ü−Öê ÃÖê ÃÖæ´Ö ‹¾ÖÓ Ã£Öã»Ö ¤üÖ−ê ÖÖë ׾֍éú×ŸÖ Ã£ÖÖ−Öߍú¸üÖ ¯Ö¸ü †¾ÖÖÓ×”ûŸÖ ¯ÖϳÖÖ¾Ö ›üÖ»ÖŸÖê Æîü †ŸÖ: ‹êÃÖÖ −ÖÆüà ú¸ü−ÖÖ “ÖÖ×Æü‹ … ´ÖãμÖ ¿Ö²¤ü : Nb-1Zr ×´ÖÁÖ¬ÖÖŸÖã, ˆ““Ö ŸÖÖ¯Ö´ÖÖ−Ö ×¸ü‹Œ™ü¸ü, ŸÖÖ¯ÖμÖÖÓס֍ú ÃÖÓÃÖÖ¬Ö−Ö, ×¾ÖÃÖ¯ÖÔÖ Thermomechanical processing of Nb­1Zr­0.1C alloy for use in  compact high temperature reactors: a first report  J.K. Chakravarttya, R. Kapoora, A.K. Suri  a Mechanical Metallurgy Division,  Materials Group, Bhabha Atomic Research Centre, Mumbai.    Abstract  Nb‐1Zr‐0.1C is a potential material for use in high temperature nuclear reactors.   Use of this alloy in components requires appropriate thermomechanical processing  to break the cast microstructure and to obtain uniformly distributed fine stable  precipitates  so  as  to  produce  the  desired  mechanical  properties  at  the  high  operating temperatures.  This report reviews the thermomechanical processing of  Nb‐1Zr‐0.1C alloy carried out over the years by other researchers and the high  temperature creep behavior of the alloy.  The hot deformation of Nb­1Zr­0.1C alloy  carried  out  at  Mechanical  Metallurgy  Division  is  also  presented  here.    From  this  review it is evident that most primary hot working studies were carried out between  1500 to 1700 °C.  The subsequent annealing treatments, which require holding at  lower temperatures of about 1100 to 1300 °C for very long times help further  transform the precipitates from coarse orthorhombic to very fine cubic.  Our studies  on Nb‐1Zr‐0.1C alloy also confirm that optimum hot working lies at temperatures  beyond 1500 °C where dynamic recrystallization initiates, and optimally around  1700 °C where dynamic recrystallization transforms the microstructure.  Working at  temperatures lower than 1000 °C may lead to the undesirable effect of both micro as  well as macro strain localization, and should be avoided.  Keywords: Nb‐1Zr alloys, high temperature reactors, thermomechanical processing,  creep.    1 1 Introduction  The development of Nb alloys for use as structural materials in nuclear reactors  was started in the early 1960’s by NASA for the specific application of nuclear  powered reactors in space vehicles referred to as Space Nuclear Power Systems (for  example see Ref. [1‐3]).  These are low powered systems of 10’s to 100’s kW  with  e an operating life of around 5 to 10 years (see Ref. [4] for overview of these systems).   The research in refractory alloys for nuclear applications did halt for a decade after  which the 1980’s saw a renewed interest in the use of refractory alloys in nuclear  fission reactors in space.  The specific requirements for alloys to be used in Space  Nuclear Powered Systems were their ability to retain strength at relatively high  temperatures (1000 to 1200 °C), long term thermal creep strength (less than 1%  strain in 7 years was the benchmark for space reactors), good compatibility with  liquid alkali metals, and low parasitic neutron cross‐section [5].  Nb alloys satisfy  these requirements and are easier to fabricate as compared to Mo and W alloys.  Ta,  which has a comparable fabricability, has the disadvantage of a higher density and a  higher neutron cross‐section as compared to Nb.  For the special application of space  nuclear power systems, the lowest density of refractory metals would be preferred,  which in this case are the Nb alloys (Nb‐1Zr, PWC‐11 and C‐103).  However, the  drawback  of  Nb  alloys  is  that  these  have  the  lowest  yield  strength  at  high  temperatures as shown in Fig. 1.  At high temperatures (1000 to 1200 ºC) the  strength of all Nb alloys fall in the same band.  Mo alloys have higher strength values  and  Mo  based  TZM  and  Ta  alloy  (T‐111)  and  have  the  highest  strengths  [5].   Although the drop in strength with increasing temperature is higher for the T‐111  and TZM, they are still stronger than Nb alloys at 1300 °C.  One of the alloys Nb‐5W‐ 2Mo‐1Zr [6] shows dynamic strain aging between 600 to 1000 °C, a region in which  no hot working should be carried out.  The UTS vs. temperature behavior of some Nb  alloys (Fig. 2) shows that for most alloys in the intermediate temperature regime  UTS increases with increasing temperature signifying dynamic strain aging.  2

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The hot deformation of Nb-1Zr-0.1C alloy carried out at Mechanical Metallurgy Division is also presented here. From this review it is evident that most
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