Analysis on Solenoidal High Temperature Superconducting Magnet using COMSOL MultiPhysics® Abhinav Kumar Department of Mechanical Engineering, Lovely Professional.

Slides:



Advertisements
Similar presentations
Electromagnetics ENGR 367
Advertisements

Chapter 30. Induction and Inductance
Q1 for JLAB’s 12 Gev/c Super High Momentum Spectrometer S.R. Lassiter, P.B. Brindza, M. J. Fowler, S.R. Milward, P. Penfold, R. Locke Q1 SHMS HMS Q2 Q3.
Superconducting Solenoid Punch Team Supercool Andy Lin Chris Kinney Naomi Kohen David Schoen.
MUTAC Review, 9 April MuCOOL and MICE Coupling Magnet Status Michael A. Green Lawrence Berkeley Laboratory Berkeley CA
Progress on the MICE Cooling Channel Solenoid Magnet System
1 The Genoa Tracker Solenoids and their Contribution toward a New Design Michael A. Green Lawrence Berkeley National Laboratory and Pasquale Fabbricatore.
CM-18 June Magnet Conductor Parameters and How They affect Conductor Selection for MICE Magnets Michael Green Lawrence Berkeley Laboratory Berkeley.
Physics 121 Practice Problem Solutions 11 Faraday’s Law of Induction
Induction and Inductance When a bar magnet moves towards the loop, there is a deflection on the ammeter and when the magnet is moved away, there is also.
TRANSFORMERS?. Effects of electric current An electric current that flows in a conductor has a number of effects: 1. HEATING The friction caused by the.
AP Physics C Montwood High School R. Casao
Magnet Options for Magnetic Intervention SC Wire Characteristics (Critical Current Density: Jc) With the advent of cusp geometry for diverting ions into.
Physics A First Course Electricity and Magnetism Chapter 17.
FAIR MT/Cryogenics, Seong Yeub Shim Beam-Tube Eddy Loss S. Y. Shim.
Bias Magnet for the Booster’s 2-nd Harmonic Cavity An attempt to evaluate the scope of work based of the existing RF design of the cavity 9/10/2015I. T.
Superconducting R&D – Now Strand and Cable R&D FERMILAB Magnet Systems Department – Now SC Materials Department (TD) HTS Insert Coil Test in External Solenoid.
Khoo Yihan | Chua Cong Yang | Park Seong Jin.  Electricity is generated in power stations at 11000V to 33000V and then stepped up to V by transformers.
Electro- magnetic Induction Lecture 3 AP Physics.
Chapter 28 Inductance; Magnetic Energy Storage. Self inductance 2 Magnetic flux Φ B ∝ current I Electric currentmagnetic fieldEMF (changing) Phenomenon.
Magnet design issues & concepts for the new injector P.Fabbricatore INFN-Genova Magnet design issues & concepts for the new injector P.Fabbricatore INFN-Genova,
Muon Cooling Channel Superconducting Magnet Systems Muon Collider Task Force Meeting on July 31, 2006 V.S. Kashikhin.
Monday, April 23, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #19 Monday, April 23, 2007 Dr. Andrew Brandt Inductance.
Cold test of SIS-300 dipole model Sergey Kozub Institute for High Energy Physics (IHEP), Protvino, Moscow region, Russia.
Reducing the Iron in the Endcap Yoke of CLIC_SiD Benoit Curé, Konrad Elsener, Hubert Gerwig, CERN CERN, June 2014 Linear Collider Detector Magnet Meeting.
HTS insert magnet design: Stack Cable Johnny Himbele, Arnaud Badel, Pascal Tixador 1.
Soumen Kar 1,2, Xiao-Fen Li 1, Venkat Selvamanickam 1, V. V. Rao 2 1 Department of Mechanical Engineering and Texas Center for Superconductivity University.
Super Fragment Separator (Super-FRS) Machine and Magnets H. Leibrock, GSI Darmstadt Review on Cryogenics, February 27th, 2012, GSI Darmstadt.
XVII SuperB Workshop and Kick Off Meeting - La Biodola (Isola d'Elba) Italy May 28 th June 2 nd 2011 P.Fabbricatore Sezione di Genova The air core magnets.
HTS and LTS Magnet Design and Prototyping for RAON
Advanced Science and Technology Letters Vol.47 (Healthcare and Nursing 2014), pp Design of Roof Type.
Test of QD0 Riccardo Musenich INFN-Genova SuperB 2 nd Collaboration Meeting Frascati, December
Ranko Ostojic AT/MEL 1.Beam heat loads 2.Magnet design issues related to heat loads.
Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits
MANUFACTURING OF MAGNETS FOR SST-1 TOKAMAK
Electricity and Magnetism
Lecture 3-7 Magnetic Energy (pg. 43 – 42)
2012 Applied Superconductivity Conference, Portland, Oregon
Fundamentals of Applied Electromagnetics
Superconducting magnet
Quench estimations of the CBM magnet
Construction and Status of Versatile Experiment Spherical Torus at SNU
When we generate power we ramp up the voltage for transmission (up to V) and then when it arrives at homes we ramp it back down for convenient use.
SiD Solenoid Status and Plans
PHYS 1444 – Section 02 Lecture #19
Electrical Engineering Department, SGSITS, Indore, INDIA
Yingshun Zhu Accelerator Center, Magnet Group
EuCARD2 WP 10.2 HTS Conductor
PHYS 1444 – Section 003 Lecture #21
Section 16-3 Electricity from Magnetism Notes
ENE 325 Electromagnetic Fields and Waves
Electric Currents from Magnetism
I. Bogdanov, S. Kozub, V. Pokrovsky, L. Shirshov,
III. Producing Electric Current
BESIII Collaboration Meeting, June 5~6, 2002, Zian Zhu
Preliminary study of HTS option for CEPC detector magnet
Producing Electric Current
Measurements (to be made): About the device (in development):
ELECTRICITY AND MAGNETISM
Revision Quiz Bowl on Electromagnetism
9. Inductance M is a geometrical factor! L is a geometrical factor!
Problems
The superconducting solenoids for the Super Charm-Tau Factory detector
Electromagnetic Induction
Quench calculations of the CBM magnet
Fabrication and Test of ϕ35mm Iron Base Superconductor Solenoid
LIQHYSMES: A novel hybrid energy storage option
Budker Institute of Nuclear Physics,
Chapter 32 Problems 6,7,9,16,29,30,31,37.
Lab: AC Circuits Integrated Science II.
Presentation transcript:

Analysis on Solenoidal High Temperature Superconducting Magnet using COMSOL MultiPhysics® Abhinav Kumar Department of Mechanical Engineering, Lovely Professional University, Phagwara, Punjab (Pb), India (1) (2) Analysis on HTS SMES Abstract: Superconducting tapes are one of the advanced materials which show their candidacy in almost every electrical engineering applications starting from the energy/power generation (Superconducting Generators) to the household/industrial distributed systems (Superconducting Transformers). Also, superconducting tapes are being exploited in energy storage applications where such tapes can be wound to form a solenoidal or toroidal shaped magnet. It has been found that solenoidal magnet consumes less superconducting material compared to toroidal thus in the present analysis solenoidal configuration has been considered where an attempt has been made to design a magnet that can store 600kJ of energy. The magnet is designed to be cooled at 20K using conduction cooling. 1st Generation HTS tape (BSCCO-2223) has been considered whose critical current at 20K is found to be 480A. Analysis shows that it will be useful to use higher currents in order to minimize the total length of the superconducting wire needed to store 600kJ of energy. A reference field of 3.5T has been employed in the design of 600kJ HTS SMES having 297mm bore diameter and inductance of 1.296H. Also, it has been assumed that the evaluated perpendicular magnetic flux density should not exceed 3T. Figure 1. Axisymmetric Model Imax (A) 336 672 1008 Imin (A) 300 Emax (MJ) 2.96 0.75 0.658 Delta E (kJ) 600 Inductance (H) 52.41 3.319 1.296 Figure 2. normB Distribution Table 1. Effect of Maximum Current on Emax and Inductance of the Coil Parameter Value Inner bore radius, r1 148.5mm Thickness of Solenoid, (r2-r1) 44.74mm Energy Stored, Emax 658kJ Deliverable Energy 600kJ Inductance of the Coil 1.296H Load Factor 0.7 Minimum Current, Imin 300A Number of SPC 396 Number of Turns of SC Tape (Approx.) 4922 Number of turns/SPC (Approx) 37 Maximum Current, Imax 1kA No. of SC tape used to support Imax 3 Critical Current Density, Jc 6.23E7 Resistivity of Vacuum (ohm*m) 0.001 Total Length of single SC Tape 15.82km Figure 3. Perpendicular B Distribution Conclusions: In the present work, electromagnetic analysis on 600kJ of HTS SMES has been done using axisymmetric 2D model. It has been found that the perpendicular magnetic flux is limited to 2.45T, thus the design is safe as the chosen field was 3T. References: M. Park et al., Analysis of magnetic field distribution and AC losses of a 600 kJ SMES, vol. 47, pp. 391–396 (2007) K. C. Seong et al., Development of a 600 kJ HTS SMES, vol. 468, pp. 2091–2095 (2008) A. Morandi, Design and Comparison of a 1-MW/5-s HTS SMES With Toroidal and Solenoidal Geometry, IEEE Transactions vol. 26, no. 4, pp. 1–6 (2016) Table 2. Parameters of HTS SMES Keep this space clear for COMSOL use. Remove this text box before submitting.