Accelerated Taylor State Plumes in SSX

Size: px
Start display at page:

Download "Accelerated Taylor State Plumes in SSX"

Transcription

1 Accelerated Taylor State Plumes in SSX Manjit Kaur Swarthmore College, Swarthmore, PA J. E. Shrock 18, J. Han 17, D. A. Schaffner & M. R. Brown Research supported by DOE OFES & ARPA-e ALPHA 24 August 2016 US-Japan Workshop on Compact Tori 2016, Hotel Irvine, Irvine, CA 92614, USA

2 Our goal Twisted Taylor state A magnetic plasma object exhibiting minimum energy state First observed in SSX lab (Gray et al., PRL, 2013) Our goal is to accelerate a Taylor state to high velocity, then stagnate and compress the object into a suitable MIF target 24 August

3 Overview of talk o System description o Un-accelerated SSX plasma o Injected into glass tube with different liners o Baseline velocity, density and temperature o Accelerated SSX plasma o Velocity predictions o Experimental progress o Summary 24 August

4 System schematic 4

5 Un-accelerated Plasma

6 Current set-up 6

7 Velocity Measurements 24 August

8 B probes installed on glass Single turn wire loops Separated by 10 cm each 24 August

9 Time of Flight measurements Time travelled by the structure at different locations 24 August

10 Plume velocity with glass 24 August

11 Resistive flux conserver SS309 foil, thickness ~ 50 μm Magnetic soak time ~ 3 μs 24 August

12 Plume velocity with resistive liner 24 August

13 Mesh flux conserver Bronze mesh, thickness ~ 450 μm, transparency ~ 42% Magnetic soak time ~ 245 μs 24 August

14 Plume velocity with mesh conserver 24 August

15 Density & Temperature measurements 24 August

16 Characterization in expansion chamber Interferometer chord, different chords of IDS and two magnetic probes also shown in the expansion chamber 24 August

17 Density of Taylor plume 24 August

18 16-channel trans-impedance amplifier circuit 24 August

19 Ion temperature Profile 24 August

20 Line shape from glass 24 August

21 Plasma production 24 August

22 Ion temperature of expansion side plasma 24 August

23 Line shape of expansion side plasma 24 August

24 Un-accelerated Taylor state Density cm 3 Mass 25 μg Volume ~15 liters Velocity ~30 km/s Kinetic energy ~10 Joules 24 August

25 o System description o Un-accelerated SSX plasma Overview of talk o Injected into glass tube with different liners o Baseline velocity, density and temperature v = 30 km/s, n cm 3, T i = 30 ev o Accelerated SSX plasma o Velocity predictions o Experimental progress o Summary 24 August

26 Accelerated Plasma

27 Acceleration with single theta pinch coil 24 August

28 Acceleration system capabilities C 1.3 μf (@100 kv) Power supply output voltage Energy stored, E C Acceleration to velocity, v acc 40 kv 1 kj 290 efficiency, v acc 145 km/s 24 August

29 Pulsed theta pinch coil Multiple parallel coaxial cable connections to reduce inductance, L 1 μh τ1 4 LC 1 μsec 24 August

30 Progress Theta pinch coil & stagnation flux conserver are ready to be installed. Assembling the different parts of the Capacitor charging and discharging circuit i.e., Bochkov switches, Ross relay, diodes, resistors, and capacitors and timing modules etc. (Ian Allfrey & Travis Valentine (TAE) are helping us with their useful suggestions) 24 August

31 Ultimate goal Four theta pinch coils will be triggered separately & sequentially to accelerate plasma to velocities over 200 km/s and to achieve compressional density over cm 3 24 August

32 Summary Taylor state characterized in new glass extension with a variety of liners, ready for stagnation experiments Theta pinch coil and accelerator test stand (1 20 kv) nearly ready using TAE components 24 August

33 Thank you

Happy New Year 2017 from SSX!

Happy New Year 2017 from SSX! Happy New Year 2017 from SSX! Here s the annual review from SSX for 2016 as well as plans for 2017. The big news this year is the arrival of Dr. Manjit Kaur as the new SSX postdoc as of May 2016. Manjit

More information

Question 1. Question 2. Question 3

Question 1. Question 2. Question 3 Question 1 Switch S in in the figure is closed at time t = 0, to begin charging an initially uncharged capacitor of capacitance C = 18.2 μf through a resistor of resistance R = 22.3 Ω. At what time (in

More information

PHYS 241 EXAM #2 November 9, 2006

PHYS 241 EXAM #2 November 9, 2006 1. ( 5 points) A resistance R and a 3.9 H inductance are in series across a 60 Hz AC voltage. The voltage across the resistor is 23 V and the voltage across the inductor is 35 V. Assume that all voltages

More information

Chapter 30 Inductance and Electromagnetic Oscillations

Chapter 30 Inductance and Electromagnetic Oscillations Chapter 30 Inductance and Electromagnetic Oscillations Units of Chapter 30 30.1 Mutual Inductance: 1 30.2 Self-Inductance: 2, 3, & 4 30.3 Energy Stored in a Magnetic Field: 5, 6, & 7 30.4 LR Circuit: 8,

More information

Turbulence Analysis of a Flux Rope Plasma on the Swarthmore Spheromak Experiment

Turbulence Analysis of a Flux Rope Plasma on the Swarthmore Spheromak Experiment Research supported by US DOE and NSF Turbulence Analysis of a Flux Rope Plasma on the Swarthmore Spheromak Experiment David Schaffner Swarthmore College, NSF Center for Magnetic Self-Organization with

More information

Alternating Current Circuits. Home Work Solutions

Alternating Current Circuits. Home Work Solutions Chapter 21 Alternating Current Circuits. Home Work s 21.1 Problem 21.11 What is the time constant of the circuit in Figure (21.19). 10 Ω 10 Ω 5.0 Ω 2.0µF 2.0µF 2.0µF 3.0µF Figure 21.19: Given: The circuit

More information

2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM FREE-RESPONSE QUESTIONS

2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM FREE-RESPONSE QUESTIONS 2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM In the circuit shown above, resistors 1 and 2 of resistance R 1 and R 2, respectively, and an inductor of inductance L are connected to a battery of emf e and

More information

Physics 196 Final Test Point

Physics 196 Final Test Point Physics 196 Final Test - 120 Point Name You need to complete six 5-point problems and six 10-point problems. Cross off one 5-point problem and one 10-point problem. 1. Two small silver spheres, each with

More information

a. Clockwise. b. Counterclockwise. c. Out of the board. d. Into the board. e. There will be no current induced in the wire

a. Clockwise. b. Counterclockwise. c. Out of the board. d. Into the board. e. There will be no current induced in the wire Physics 1B Winter 2012: Final Exam For Practice Version A 1 Closed book. No work needs to be shown for multiple-choice questions. The first 10 questions are the makeup Quiz. The remaining questions are

More information

Assessment Schedule 2015 Physics: Demonstrate understanding of electrical systems (91526)

Assessment Schedule 2015 Physics: Demonstrate understanding of electrical systems (91526) NCEA Level 3 Physics (91526) 2015 page 1 of 6 Assessment Schedule 2015 Physics: Demonstrate understanding of electrical systems (91526) Evidence Q Evidence Achievement Achievement with Merit Achievement

More information

Version 001 CIRCUITS holland (1290) 1

Version 001 CIRCUITS holland (1290) 1 Version CIRCUITS holland (9) This print-out should have questions Multiple-choice questions may continue on the next column or page find all choices before answering AP M 99 MC points The power dissipated

More information

ε induced Review: Self-inductance 20.7 RL Circuits Review: Self-inductance B induced Announcements

ε induced Review: Self-inductance 20.7 RL Circuits Review: Self-inductance B induced Announcements Announcements WebAssign HW Set 7 due this Friday Problems cover material from Chapters 20 and 21 We re skipping Sections 21.1-21.7 (alternating current circuits) Review: Self-inductance induced ε induced

More information

Exam 3--PHYS 102--S14

Exam 3--PHYS 102--S14 Name: Exam 3--PHYS 102--S14 Multiple Choice Identify the choice that best completes the statement or answers the question. 1. Which of these statements is always true? a. resistors in parallel have the

More information

Inductance, RL and RLC Circuits

Inductance, RL and RLC Circuits Inductance, RL and RLC Circuits Inductance Temporarily storage of energy by the magnetic field When the switch is closed, the current does not immediately reach its maximum value. Faraday s law of electromagnetic

More information

Chapter 30 INDUCTANCE. Copyright 2012 Pearson Education Inc.

Chapter 30 INDUCTANCE. Copyright 2012 Pearson Education Inc. Chapter 30 INDUCTANCE Goals for Chapter 30 To learn how current in one coil can induce an emf in another unconnected coil To relate the induced emf to the rate of change of the current To calculate the

More information

An Optimised High Current Impulse Source

An Optimised High Current Impulse Source An Optimised High Current Impulse Source S. Kempen, D. Peier Institute of High Voltage Engineering, University of Dortmund, Germany Abstract Starting from a predefined 8/0 µs impulse current, the design

More information

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS Name of contact person: Surender Kumar Sharma Name of other contributors: R.

More information

The next two questions pertain to the situation described below. Consider a parallel plate capacitor with separation d:

The next two questions pertain to the situation described below. Consider a parallel plate capacitor with separation d: PHYS 102 Exams Exam 2 PRINT (A) The next two questions pertain to the situation described below. Consider a parallel plate capacitor with separation d: It is connected to a battery with constant emf V.

More information

Physics 126 Fall 2004 Practice Exam 1. Answer will be posted about Oct. 5.

Physics 126 Fall 2004 Practice Exam 1. Answer will be posted about Oct. 5. Physics 126 Fall 2004 Practice Exam 1. Answer will be posted about Oct. 5. 1. Which one of the following statements best explains why tiny bits of paper are attracted to a charged rubber rod? A) Paper

More information

AP Physics C. Inductance. Free Response Problems

AP Physics C. Inductance. Free Response Problems AP Physics C Inductance Free Response Problems 1. Two toroidal solenoids are wounded around the same frame. Solenoid 1 has 800 turns and solenoid 2 has 500 turns. When the current 7.23 A flows through

More information

Discharge Cell Design. Some initial explorations, considerations and open questions

Discharge Cell Design. Some initial explorations, considerations and open questions Discharge Cell Design Some initial explorations, considerations and open questions Modelling plasma discharge circuit demands Based on paper from SPARC-LAB experiment (Nuc. Instrum Meth A 2015) Design

More information

Induction_P1. 1. [1 mark]

Induction_P1. 1. [1 mark] Induction_P1 1. [1 mark] Two identical circular coils are placed one below the other so that their planes are both horizontal. The top coil is connected to a cell and a switch. The switch is closed and

More information

Physics 240 Fall 2005: Exam #3. Please print your name: Please list your discussion section number: Please list your discussion instructor:

Physics 240 Fall 2005: Exam #3. Please print your name: Please list your discussion section number: Please list your discussion instructor: Physics 240 Fall 2005: Exam #3 Please print your name: Please list your discussion section number: Please list your discussion instructor: Form #1 Instructions 1. Fill in your name above 2. This will be

More information

P202 Practice Exam 2 Spring 2004 Instructor: Prof. Sinova

P202 Practice Exam 2 Spring 2004 Instructor: Prof. Sinova P202 Practice Exam 2 Spring 2004 Instructor: Prof. Sinova Name: Date: (5)1. How many electrons flow through a battery that delivers a current of 3.0 A for 12 s? A) 4 B) 36 C) 4.8 10 15 D) 6.4 10 18 E)

More information

RC Circuits (32.9) Neil Alberding (SFU Physics) Physics 121: Optics, Electricity & Magnetism Spring / 1

RC Circuits (32.9) Neil Alberding (SFU Physics) Physics 121: Optics, Electricity & Magnetism Spring / 1 (32.9) We have only been discussing DC circuits so far. However, using a capacitor we can create an RC circuit. In this example, a capacitor is charged but the switch is open, meaning no current flows.

More information

PRACTICE EXAM 1 for Midterm 2

PRACTICE EXAM 1 for Midterm 2 PRACTICE EXAM 1 for Midterm 2 Multiple Choice Questions 1) The figure shows three identical lightbulbs connected to a battery having a constant voltage across its terminals. What happens to the brightness

More information

Do not fill out the information below until instructed to do so! Name: Signature: Section Number:

Do not fill out the information below until instructed to do so! Name: Signature:   Section Number: Do not fill out the information below until instructed to do so! Name: Signature: E-mail: Section Number: No calculators are allowed in the test. Be sure to put a box around your final answers and clearly

More information

Inductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits

Inductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits Inductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the timevarying

More information

PROTEAN : Neutral Entrainment Thruster Demonstration

PROTEAN : Neutral Entrainment Thruster Demonstration PROTEAN : Neutral Entrainment Thruster Demonstration Dr. David Kirtley Dr. George Votroubek Dr. Anthony Pancotti Mr. Michael Pfaff Mr. George Andexler MSNW LLC - Principle Investigator -Dynamic Accelerator

More information

RC Studies Relaxation Oscillator

RC Studies Relaxation Oscillator RC Studies Relaxation Oscillator Introduction A glass tube containing neon gas will give off its characteristic light when the voltage across the tube exceeds a certain value. The value corresponds to

More information

The electrical Discharge Characteristics of the 3.5 KJ Electrothermal Plasma Gun Experiment

The electrical Discharge Characteristics of the 3.5 KJ Electrothermal Plasma Gun Experiment The electrical Discharge Characteristics of the 3.5 KJ Electrothermal Plasma Gun Experiment F. Diab, G. M. El-Aragi, G. M. El-Kashef and A. H. Saudy* Plasma and Nuclear fusion Department, AEA, Cairo, Egypt

More information

Select the response that best answers the given statement. Be sure to write all final multiple choice answers on your Scantron answer sheet.

Select the response that best answers the given statement. Be sure to write all final multiple choice answers on your Scantron answer sheet. Chapters 15-30 PHYS 1402 - Brooks This practice test is similar to the actual final. The final exam will focus on questions involving solving problems, and not so much on conceptual questions. The final

More information

Louisiana State University Physics 2102, Exam 2, March 5th, 2009.

Louisiana State University Physics 2102, Exam 2, March 5th, 2009. PRINT Your Name: Instructor: Louisiana State University Physics 2102, Exam 2, March 5th, 2009. Please be sure to PRINT your name and class instructor above. The test consists of 4 questions (multiple choice),

More information

Physics 6B Summer 2007 Final

Physics 6B Summer 2007 Final Physics 6B Summer 2007 Final Question 1 An electron passes through two rectangular regions that contain uniform magnetic fields, B 1 and B 2. The field B 1 is stronger than the field B 2. Each field fills

More information

Active Stability Control of a High-Beta Self-Organized Compact Torus

Active Stability Control of a High-Beta Self-Organized Compact Torus 1 ICC/P5-01 Active Stability Control of a High-Beta Self-Organized Compact Torus T. Asai 1), Ts. Takahashi 1), H. Matsunaga 1), H. Itagaki 1), Y. Matsuzawa 1), Y. Hirano 1), To. Takahashi 2), M. Inomoto

More information

Nanosecond-scale Processes in a Plasma Pilot for Ignition and Flame Control

Nanosecond-scale Processes in a Plasma Pilot for Ignition and Flame Control Nanosecond-scale Processes in a Plasma Pilot for Ignition and Flame Control Yu. D. Korolev, I. B. Matveev Institute of High Current Electronics, 634055 Tomsk, Russia Applied Plasma Technologies, Falls

More information

Flow dynamics and plasma heating of spheromaks in SSX

Flow dynamics and plasma heating of spheromaks in SSX Flow dynamics and plasma heating of spheromaks in SSX M. R. Brown and C. D. Cothran, D. Cohen, J. Horwitz, and V. Chaplin Department of Physics and Astronomy Center for Magnetic Self Organization Swarthmore

More information

Application of Physics II for. Final Exam

Application of Physics II for. Final Exam Application of Physics II for Final Exam Question 1 Four resistors are connected as shown in Figure. (A)Find the equivalent resistance between points a and c. (B)What is the current in each resistor if

More information

Ch. 3. Pulsed and Water Cooled Magnets. T. J. Dolan. Magnetic field calculations

Ch. 3. Pulsed and Water Cooled Magnets. T. J. Dolan. Magnetic field calculations Ch. 3. Pulsed and Water Cooled Magnets T. J. Dolan Magnetic field calculations Coil forces RLC circuit equations Distribution of J and B Energy storage Switching and transmission Magnetic flux compression

More information

Chapter 30. Inductance

Chapter 30. Inductance Chapter 30 Inductance Self Inductance When a time dependent current passes through a coil, a changing magnetic flux is produced inside the coil and this in turn induces an emf in that same coil. This induced

More information

Physics 212 Midterm 2 Form A

Physics 212 Midterm 2 Form A 1. A wire contains a steady current of 2 A. The charge that passes a cross section in 2 s is: A. 3.2 10-19 C B. 6.4 10-19 C C. 1 C D. 2 C E. 4 C 2. In a Physics 212 lab, Jane measures the current versus

More information

Practice Exam 1. Necessary Constants and Equations: Electric force (Coulomb s Law): Electric field due to a point charge:

Practice Exam 1. Necessary Constants and Equations: Electric force (Coulomb s Law): Electric field due to a point charge: Practice Exam 1 Necessary Constants and Equations: Electric force (Coulomb s Law): Electric field due to a point charge: Electric potential due to a point charge: Electric potential energy: Capacitor energy:

More information

Large Plasma Device (LAPD)

Large Plasma Device (LAPD) Large Plasma Device (LAPD) Over 450 Access ports Computer Controlled Data Acquisition Microwave Interferometers Laser Induced Fluorescence DC Magnetic Field: 0.05-4 kg, variable on axis Highly Ionized

More information

PHYSICS HIGHER LEVEL

PHYSICS HIGHER LEVEL *P16* PRE-LEAVING CERTIFICATE EXAMINATION, 2011 PHYSICS HIGHER LEVEL TIME: 3 HOURS Answer three questions from section A and five questions from section B. Page 1 of 9 SECTION A (120 marks) Answer three

More information

Additional Heating Experiments of FRC Plasma

Additional Heating Experiments of FRC Plasma Additional Heating Experiments of FRC Plasma S. Okada, T. Asai, F. Kodera, K. Kitano, T. Suzuki, K. Yamanaka, T. Kanki, M. Inomoto, S. Yoshimura, M. Okubo, S. Sugimoto, S. Ohi, S. Goto, Plasma Physics

More information

Question 1. (Marks 16)

Question 1. (Marks 16) 5 Question 1. (Marks 16) Consider the circuit shown in the figure, where C 1 = 6.00µF, C 2 = 3.00µF, and V = 20.0V. Capacitor C 1 is first charged by closing switch S 1. Switch S 1 is then opened, and

More information

Experiment FT1: Measurement of Dielectric Constant

Experiment FT1: Measurement of Dielectric Constant Experiment FT1: Measurement of Dielectric Constant Name: ID: 1. Objective: (i) To measure the dielectric constant of paper and plastic film. (ii) To examine the energy storage capacity of a practical capacitor.

More information

Physics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:

Physics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Physics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Closed book. No work needs to be shown for multiple-choice questions. 1. A charge of +4.0 C is placed at the origin. A charge of 3.0 C

More information

Louisiana State University Physics 2102, Exam 3, November 11, 2010.

Louisiana State University Physics 2102, Exam 3, November 11, 2010. Name: Instructor: Louisiana State University Physics 2102, Exam 3, November 11, 2010. Please be sure to write your name and class instructor above. The test consists of 3 questions (multiple choice), and

More information

LR Circuits. . The voltage drop through both resistors will equal. Hence 10 1 A

LR Circuits. . The voltage drop through both resistors will equal. Hence 10 1 A The diagram shows a classic R circuit, containing both resistors and inductors. The switch shown is initially connected to neither terminal, and is then thrown to position a at time t = 0. R Circuits E

More information

APPLICATION OF DETONATION TO PROPULSION. S. M. Frolov, V. Ya. Basevich, and V. S. Aksenov

APPLICATION OF DETONATION TO PROPULSION. S. M. Frolov, V. Ya. Basevich, and V. S. Aksenov APPLICATION OF DETONATION TO PROPULSION COMBUSTION CHAMBER WITH INTERMITTENT GENERATION AND AMPLIFICATION OF PROPAGATING REACTIVE SHOCKS S. M. Frolov, V. Ya. Basevich, and V. S. Aksenov N. N. Semenov Institute

More information

Equilibrium Evolution in the ZaP Flow Z-Pinch

Equilibrium Evolution in the ZaP Flow Z-Pinch Equilibrium Evolution in the ZaP Flow Z-Pinch U. Shumlak, B.A. Nelson, C.S. Adams, D.J. Den Hartog, R.P. Golingo, S. L. Jackson, S.D. Knecht, J. Pasko, and D.T. Schmuland University of Washington, Seattle

More information

Louisiana State University Physics 2102, Exam 3 April 2nd, 2009.

Louisiana State University Physics 2102, Exam 3 April 2nd, 2009. PRINT Your Name: Instructor: Louisiana State University Physics 2102, Exam 3 April 2nd, 2009. Please be sure to PRINT your name and class instructor above. The test consists of 4 questions (multiple choice),

More information

PHY 101 Practice Exam III Monday, November 27, 2:15-3:35PM

PHY 101 Practice Exam III Monday, November 27, 2:15-3:35PM 1 PHY 101 Practice Exam III Monday, November 27, 2:15-3:35PM Please be sure to show your work where it is requested. If no work is shown where it is requested, you will not receive any points. Partial

More information

Physics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:

Physics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Physics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Closed book. No work needs to be shown for multiple-choice questions. 1. Four charges are at the corners of a square, with B and C on opposite

More information

Good Luck! Mlanie LaRoche-Boisvert - Electromagnetism Electromagnetism and Optics - Winter PH. Electromagnetism and Optics - Winter PH

Good Luck! Mlanie LaRoche-Boisvert - Electromagnetism Electromagnetism and Optics - Winter PH. Electromagnetism and Optics - Winter PH 1 Notes: 1. To submit a problem, just click the Submit button under it. The Submit All button is not necessary. 2. A problem accepted as correct by CAPA will be highlighted in green. Once you see this,

More information

Active Figure 32.3 (SLIDESHOW MODE ONLY)

Active Figure 32.3 (SLIDESHOW MODE ONLY) RL Circuit, Analysis An RL circuit contains an inductor and a resistor When the switch is closed (at time t = 0), the current begins to increase At the same time, a back emf is induced in the inductor

More information

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Lecture 5: Electrical and Electromagnetic System Components The objective of this

More information

PLK VICWOOD K.T. CHONG SIXTH FORM COLLEGE Form Six Second Term Final Examination ( ) Physics A-Level Paper 1 Question/Answer Book A

PLK VICWOOD K.T. CHONG SIXTH FORM COLLEGE Form Six Second Term Final Examination ( ) Physics A-Level Paper 1 Question/Answer Book A 05-06/F. 6 Final Exam/AL Physics/Paper 1/P.1 PLK VICWOOD K.T. CHONG SIXTH FORM COLLEGE Form Six Second Term Final Examination (2005-2006) A Physics A-Level Paper 1 Question/Answer Book A Time Allowed:

More information

PhysicsAndMathsTutor.com 1

PhysicsAndMathsTutor.com 1 PhysicsAndMathsTutor.com 1 Q1. A 400 μf capacitor is charged so that the voltage across its plates rises at a constant rate from 0 V to 4.0 V in 20 s. What current is being used to charge the capacitor?

More information

Part 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is

Part 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is 1 Part 4: Electromagnetism 4.1: Induction A. Faraday's Law The magnetic flux through a loop of wire is Φ = BA cos θ B A B = magnetic field penetrating loop [T] A = area of loop [m 2 ] = angle between field

More information

Chapter 32. Inductance

Chapter 32. Inductance Chapter 32 Inductance Joseph Henry 1797 1878 American physicist First director of the Smithsonian Improved design of electromagnet Constructed one of the first motors Discovered self-inductance Unit of

More information

Inductance, RL Circuits, LC Circuits, RLC Circuits

Inductance, RL Circuits, LC Circuits, RLC Circuits Inductance, R Circuits, C Circuits, RC Circuits Inductance What happens when we close the switch? The current flows What does the current look like as a function of time? Does it look like this? I t Inductance

More information

ELECTRO MAGNETIC INDUCTION

ELECTRO MAGNETIC INDUCTION ELECTRO MAGNETIC INDUCTION 1) A Circular coil is placed near a current carrying conductor. The induced current is anti clock wise when the coil is, 1. Stationary 2. Moved away from the conductor 3. Moved

More information

Influence of Electrode Configuration of a Liquid Propellant PPT on its Performance

Influence of Electrode Configuration of a Liquid Propellant PPT on its Performance Influence of Electrode Configuration of a Liquid Propellant PPT on its Performance IEPC-- /ISTS--b- Presented at Joint Conference of th International Symposium on Space Technology and Science th International

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2003 Experiment 17: RLC Circuit (modified 4/15/2003) OBJECTIVES

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2003 Experiment 17: RLC Circuit (modified 4/15/2003) OBJECTIVES MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8. Spring 3 Experiment 7: R Circuit (modified 4/5/3) OBJECTIVES. To observe electrical oscillations, measure their frequencies, and verify energy

More information

1. (a) On the diagram below, draw the magnetic field pattern around a long straight currentcarrying

1. (a) On the diagram below, draw the magnetic field pattern around a long straight currentcarrying 1. (a) On the diagram below, draw the magnetic field pattern around a long straight currentcarrying conductor. current-carrying wire The diagram below shows a coil consisting of two loops of wire. The

More information

Physics 240 Fall 2005: Exam #3 Solutions. Please print your name: Please list your discussion section number: Please list your discussion instructor:

Physics 240 Fall 2005: Exam #3 Solutions. Please print your name: Please list your discussion section number: Please list your discussion instructor: Physics 4 Fall 5: Exam #3 Solutions Please print your name: Please list your discussion section number: Please list your discussion instructor: Form #1 Instructions 1. Fill in your name above. This will

More information

Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current.

Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current. Inductance Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current. Basis of the electrical circuit element called an

More information

EXEMPLAR NATIONAL CERTIFICATE (VOCATIONAL) ELECTRICAL PRINCIPLES AND PRACTICE NQF LEVEL 3 ( ) (X-Paper) 09:00 12:00

EXEMPLAR NATIONAL CERTIFICATE (VOCATIONAL) ELECTRICAL PRINCIPLES AND PRACTICE NQF LEVEL 3 ( ) (X-Paper) 09:00 12:00 NATIONAL CERTIFICATE (VOCATIONAL) ELECTRICAL PRINCIPLES AND PRACTICE NQF LEVEL 3 2008 (12041002) (X-Paper) 09:00 12:00 EXEMPLAR This question paper consists of 7 pages. EXEMPLAR -2- NC(V) TIME: 3 HOURS

More information

PES 1120 Spring 2014, Spendier Lecture 35/Page 1

PES 1120 Spring 2014, Spendier Lecture 35/Page 1 PES 0 Spring 04, Spendier Lecture 35/Page Today: chapter 3 - LC circuits We have explored the basic physics of electric and magnetic fields and how energy can be stored in capacitors and inductors. We

More information

fusion production of elements in stars, 345

fusion production of elements in stars, 345 I N D E X AC circuits capacitive reactance, 278 circuit frequency, 267 from wall socket, 269 fundamentals of, 267 impedance in general, 283 peak to peak voltage, 268 phase shift in RC circuit, 280-281

More information

Physics Investigation 10 Teacher Manual

Physics Investigation 10 Teacher Manual Physics Investigation 10 Teacher Manual Observation When a light bulb is connected to a number of charged capacitors, it lights up for different periods of time. Problem What does the rate of discharging

More information

Lab 4 - First Order Transient Response of Circuits

Lab 4 - First Order Transient Response of Circuits Lab 4 - First Order Transient Response of Circuits Lab Performed on October 22, 2008 by Nicole Kato, Ryan Carmichael, and Ti Wu Report by Ryan Carmichael and Nicole Kato E11 Laboratory Report Submitted

More information

Coulomb s constant k = 9x10 9 N m 2 /C 2

Coulomb s constant k = 9x10 9 N m 2 /C 2 1 Part 2: Electric Potential 2.1: Potential (Voltage) & Potential Energy q 2 Potential Energy of Point Charges Symbol U mks units [Joules = J] q 1 r Two point charges share an electric potential energy

More information

LABORATORY 4 ELECTRIC CIRCUITS I. Objectives

LABORATORY 4 ELECTRIC CIRCUITS I. Objectives LABORATORY 4 ELECTRIC CIRCUITS I Objectives to be able to discuss potential difference and current in a circuit in terms of electric field, work per unit charge and motion of charges to understand that

More information

Chapter 23 Magnetic Flux and Faraday s Law of Induction

Chapter 23 Magnetic Flux and Faraday s Law of Induction Chapter 23 Magnetic Flux and Faraday s Law of Induction 1 Overview of Chapter 23 Induced Electromotive Force Magnetic Flux Faraday s Law of Induction Lenz s Law Mechanical Work and Electrical Energy Generators

More information

Happy New Year 2019 from SSX!

Happy New Year 2019 from SSX! Happy New Year 2019 from SSX! Here s the annual review from SSX for 2018 as well as plans for 2019. This marks the 25 th year of SSX (we started in 1994), and I m anticipating a lot of changes this year.

More information

P114 University of Rochester NAME S. Manly Spring 2010

P114 University of Rochester NAME S. Manly Spring 2010 Exam 2 (March 23, 2010) Please read the problems carefully and answer them in the space provided. Write on the back of the page, if necessary. Show your work where indicated. Problem 1 ( 8 pts): In each

More information

Flow and dynamo measurements in the HIST double pulsing CHI experiment

Flow and dynamo measurements in the HIST double pulsing CHI experiment Innovative Confinement Concepts (ICC) & US-Japan Compact Torus (CT) Plasma Workshop August 16-19, 211, Seattle, Washington HIST Flow and dynamo measurements in the HIST double pulsing CHI experiment M.

More information

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT Chapter 31: ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT 1 A charged capacitor and an inductor are connected in series At time t = 0 the current is zero, but the capacitor is charged If T is the

More information

Double Null Merging Start-up Experiments in the University of Tokyo Spherical Tokamak

Double Null Merging Start-up Experiments in the University of Tokyo Spherical Tokamak 1 EXS/P2-19 Double Null Merging Start-up Experiments in the University of Tokyo Spherical Tokamak T. Yamada 1), R. Imazawa 2), S. Kamio 1), R. Hihara 1), K. Abe 1), M. Sakumura 1), Q. H. Cao 1), H. Sakakita

More information

Behavior of Compact Toroid Injected into the External Magnetic Field

Behavior of Compact Toroid Injected into the External Magnetic Field Behavior of Compact Toroid Injected into the External Magnetic Field M. Nagata 1), N. Fukumoto 1), H. Ogawa 2), T. Ogawa 2), K. Uehara 2), H. Niimi 3), T. Shibata 2), Y. Suzuki 4), Y. Miura 2), N. Kayukawa

More information

The output voltage is given by,

The output voltage is given by, 71 The output voltage is given by, = (3.1) The inductor and capacitor values of the Boost converter are derived by having the same assumption as that of the Buck converter. Now the critical value of the

More information

SPS Presents: A Cosmic Lunch!

SPS Presents: A Cosmic Lunch! SPS Presents: A Cosmic Lunch! Who: Dr. Brown will be speaking about Evolution of the Elements: from Periodic table to Standard Model and Beyond! When: October 7 th at am Where: CP 79 (by the front office)

More information

Capacitors. How long did the LED remain lit when the capacitors were connected in series?

Capacitors. How long did the LED remain lit when the capacitors were connected in series? Labs for College Physics - Electricity and Magnetism Worksheet Lab 2-1 Capacitors As you work through the steps in the lab procedure, record your experimental values and the results on this worksheet.

More information

Electromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.

Electromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3. Electromagnetic Oscillations and Alternating Current 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3. RLC circuit in AC 1 RL and RC circuits RL RC Charging Discharging I = emf R

More information

Electric Rocket Engine System R&D

Electric Rocket Engine System R&D Electric Rocket Engine System R&D In PROITERES, a powered flight by an electric rocket engine is planed; that is, orbital transfer will be carried out with a pulsed plasma thruster (PPT). We introduce

More information

Performance Characteristics of Electrothermal Pulsed Plasma Thrusters with Insulator-Rod-Arranged Cavities and Teflon-Alternative Propellants

Performance Characteristics of Electrothermal Pulsed Plasma Thrusters with Insulator-Rod-Arranged Cavities and Teflon-Alternative Propellants Performance Characteristics of Electrothermal Pulsed Plasma Thrusters with Insulator-Rod-Arranged Cavities and Teflon-Alternative Propellants IEPC-2007-337 Presented at the 30 th International Electric

More information

PHYSICS 2B FINAL EXAM ANSWERS WINTER QUARTER 2010 PROF. HIRSCH MARCH 18, 2010 Problems 1, 2 P 1 P 2

PHYSICS 2B FINAL EXAM ANSWERS WINTER QUARTER 2010 PROF. HIRSCH MARCH 18, 2010 Problems 1, 2 P 1 P 2 Problems 1, 2 P 1 P 1 P 2 The figure shows a non-conducting spherical shell of inner radius and outer radius 2 (i.e. radial thickness ) with charge uniformly distributed throughout its volume. Prob 1:

More information

Physics by Discovery Standards (2nd Semester)

Physics by Discovery Standards (2nd Semester) Physics by Discovery Standards 2017-18 (2nd Semester) 11. Newton's Law of Universal Gravitation UG I can apply the Law of Universal Gravitation Reason about how doubling distance, masses, etc. affect the

More information

Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance

Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance Lesson 7 Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance Oscillations in an LC Circuit The RLC Circuit Alternating Current Electromagnetic

More information

Effects of Inductive Coil Geometry in the Conical Theta Pinch Faraday Accelerator with Radio Frequency Assisted Discharge

Effects of Inductive Coil Geometry in the Conical Theta Pinch Faraday Accelerator with Radio Frequency Assisted Discharge 45th AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit 2-5 August 2009, Denver, Colorado AIAA 2009-5448 Effects of Inductive Coil Geometry in the Conical Theta Pinch Faraday Accelerator with Radio

More information

Exam 2 Fall 2014

Exam 2 Fall 2014 1 95.144 Exam 2 Fall 2014 Section instructor Section number Last/First name Last 3 Digits of Student ID Number: Show all work. Show all formulas used for each problem prior to substitution of numbers.

More information

Magnetized Target Fusion: Prospects for low-cost fusion energy

Magnetized Target Fusion: Prospects for low-cost fusion energy Magnetized Target Fusion: Prospects for low-cost fusion energy Richard E. Siemon a, Peter J. Turchi a, Daniel C. Barnes a, James H. Degnan b, Paul Parks c, Dmitri D. Ryutov d, Francis Y. Thio e a) Los

More information

A Level Physics B (Advancing Physics) H557/03 Practical skills in physics Sample Question Paper SPECIMEN

A Level Physics B (Advancing Physics) H557/03 Practical skills in physics Sample Question Paper SPECIMEN A Level Physics B (Advancing Physics) H557/03 Practical skills in physics Sample Question Paper Date Morning/Afternoon Time allowed: 1 hour 30 minutes You must have: the Data, Formulae and Relationships

More information

ECE 241L Fundamentals of Electrical Engineering. Experiment 5 Transient Response

ECE 241L Fundamentals of Electrical Engineering. Experiment 5 Transient Response ECE 241L Fundamentals of Electrical Engineering Experiment 5 Transient Response NAME PARTNER A. Objectives: I. Learn how to use the function generator and oscilloscope II. Measure step response of RC and

More information

Alternating Currents. The power is transmitted from a power house on high voltage ac because (a) Electric current travels faster at higher volts (b) It is more economical due to less power wastage (c)

More information

Pretest ELEA1831 Module 11 Units 1& 2 Inductance & Capacitance

Pretest ELEA1831 Module 11 Units 1& 2 Inductance & Capacitance Pretest ELEA1831 Module 11 Units 1& 2 Inductance & Capacitance 1. What is Faraday s Law? Magnitude of voltage induced in a turn of wire is proportional to the rate of change of flux passing through that

More information

UNIVERSITY OF CAMBRIDGE INTERNATIONAL EXAMINATIONS General Certificate of Education Advanced Level

UNIVERSITY OF CAMBRIDGE INTERNATIONAL EXAMINATIONS General Certificate of Education Advanced Level UNIVERSITY OF CAMBRIDGE INTERNATIONAL EXAMINATIONS General Certificate of Education Advanced Level *2809002895* PHYSICS 9702/04 Paper 4 A2 Structured Questions October/November 2007 1 hour 45 minutes Candidates

More information