Determination of suitable driver materials for electromagnetic sheet metal forming

Similar documents
Induction Heating: fundamentals

Electromagnetic Testing (ET)

NEW SOUTH WALES DEPARTMENT OF EDUCATION AND TRAINING Manufacturing and Engineering ESD. Sample Examination EA605

Application Of Faraday s Law

Induction_P1. 1. [1 mark]

Numerical Simulation and Experimental Study of Electromagnetic Forming

Electromagnetic Forming Process Analysis Based on Coupled Simulations of Electromagnetic Analysis and Structural Analysis

Tutorial Sheet IV. Fig. IV_2.

Electromagnetic Induction Practice Problems Homework PSI AP Physics B

An Optimised High Current Impulse Source

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION

COLLEGE PHYSICS Chapter 23 ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES

Fig. 2.1 I =... A [2] Suggest why it would be impossible for overhead cables carrying an alternating current to float in the Earth s magnetic field.

Revision Guide for Chapter 15

October 23. Physics 272. Fall Prof. Philip von Doetinchem

Capacitors. Typical electrical characteristics of metallized polyester capacitors KEU. Type KEU Metallized polyester capacitors

REVIEW SESSION. Midterm 2

Electromagnetic Induction

FARADAY S AND LENZ LAW B O O K P G

Physics 1402: Lecture 18 Today s Agenda

Induction. Chapter 29. PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman. Lectures by James Pazun

CERN ACCELERATOR SCHOOL Power Converters. Passive components. Prof. Alfred Rufer

Faraday's Law ds B B G G ΦB B ds Φ ε = d B dt

Sliding Conducting Bar

Revision Guide for Chapter 15

1814. Optimized design to improve the function of a magnetic pulse forming device

CHAPTER 5 ELECTROMAGNETIC INDUCTION

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Electronics & Communication Engineering

Slide 1 / 24. Electromagnetic Induction 2011 by Bryan Pflueger

Comparison Between Experimental and Numerical Results of Electromagnetic Forming Processes

Electromagnetic Induction

Lenz s Law (Section 22.5)

Measurements in Mechatronic design. Transducers

Physics 201. Professor P. Q. Hung. 311B, Physics Building. Physics 201 p. 1/1

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

Lecture 30: WED 04 NOV

MCE380: Measurements and Instrumentation Lab. Chapter 5: Electromechanical Transducers

Modelling, Simulation and Temperature Effect Analysis of Mutual Induction based High Temperature Level Sensor using COMSOL Multiphysics

NUMERICAL SIMULATION OF ELECTROMAGNETIC FORMING PROCESS USING A COMBINATION OF BEM AND FEM

Faraday s Law. Underpinning of Much Technology

Digital Fluxmeter CYHT700SP

Our goal for today. 1. To go over the pictorial approach to Lenz s law.

Magnetic Fields

Electromagnetic Induction

ELECTROMAGNETIC METAL FORMING

INVERSION OF TRANSIENT EDDY-CURRENT SIGNALS FOR THE DETERMINATION OF CONDUCTING PLATE PARAMETERS

The initial magnetization curve shows the magnetic flux density that would result when an increasing magnetic field is applied to an initially

FXA 2008 Φ = BA. Candidates should be able to : Define magnetic flux. Define the weber (Wb). Select and use the equation for magnetic flux :

Electromagnetic Induction

Physics 1402: Lecture 19 Today s Agenda

C. Incorrect! Use the formula for magnetic flux. This is the product of magnetic field, times area, times the angle between them.

Pulling or pushing a wire through a magnetic field creates a motional EMF in the wire and a current I = E/R in the circuit.

A Generator! Neil Alberding (SFU Physics) Physics 121: Optics, Electricity & Magnetism Spring / 22

Amir Hossein Parvardi 1

General Physics II. Electromagnetic Induction and Electromagnetic Waves

Shielding Tutorial Gentex EME Lab

Prince Sattam bin Abdulaziz University College of Engineering. Electrical Engineering Department EE 3360 Electrical Machines (II)

Update On The Electromagnetism Module In LS-DYNA

1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. magnetic. flux linkage / Wb-turns 1.

Simulation and verification of

Fachgebiet Leistungselektronik und Elektrische Antriebstechnik. Test Examination: Mechatronics and Electrical Drives

Thermal analysis of magnetic shields for induction heating P. Sergeant 1,2 D. Hectors 3 L. Dupré 1 K. Van Reusel 1,3

Definition Application of electrical machines Electromagnetism: review Analogies between electric and magnetic circuits Faraday s Law Electromagnetic

RLC Circuit (3) We can then write the differential equation for charge on the capacitor. The solution of this differential equation is

Inductance, RL and RLC Circuits

Exam 3 Solutions. The induced EMF (magnitude) is given by Faraday s Law d dt dt The current is given by

Physics (Theory) There are 30 questions in total. Question Nos. 1 to 8 are very short answer type questions and carry one mark each.

Motional Electromotive Force

External high-quality-factor resonator tunes up nuclear magnetic resonance

Michael Faraday. Chapter 31. EMF Produced by a Changing Magnetic Field, 1. Induction. Faraday s Law

1 (a) Define magnetic flux [1]

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring Experiment 5: Faraday s Law

Lecture 35. PHYC 161 Fall 2016

Chapter 5. Electromagnetic Induction

ELECTROMAMAGNETIC INDUCTION EDDY CURRENTS VISUAL PHYSICS ONLINE

DATA SHEET WIEGAND WIRE SENSOR WS-UTS-4-U0, WS-UFS-4-U0

Magnetic Pulse Forming: Simulation and Experiments for high-speed forming processes

Physics Notes for Class 12 chapter 6 ELECTROMAGNETIC I NDUCTION

AAST/AEDT. Electromagnetic Induction. If the permanent magnet is at rest, then - there is no current in a coil.

ELECTROMAGNETIC FIELD

However, in matter, magnetic induction depends on magnetization M in the following way:

Physics 132: Lecture 15 Elements of Physics II Agenda for Today

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

PHYSICAL SCIENCES: PAPER I

Electric Machines I Three Phase Induction Motor. Dr. Firas Obeidat

Ferromagnetism. we saw that with the propane torch on Thursday

UNIT-III Maxwell's equations (Time varying fields)

Faraday s Law of Electromagnetic Induction

Tactics: Evaluating line integrals

Magnetic inductance & Solenoids. P.Ravindran, PHY041: Electricity & Magnetism 22 February 2013: Magnetic inductance, and Solenoid

AGENERAL approach for the calculation of iron loss in

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT

Don t Copy This. Michael Faraday 3/1/13. Chapter 25: EM Induction and EM Waves. Key Terms:

TRANSFORMERS B O O K P G

EC T32 - ELECTRICAL ENGINEERING

Numerical Simulation and Experimental Study for Magnetic Pulse Welding Process on AA6061-T6 and Cu101 Sheet

Preview of Period 17: Induction Motors and Transformers

force per unit length

EN Power Electronics and Machines

DHANALAKSHMI COLLEGE OF ENGINEERING DEPARTMENT OF EEE PART A. 1. Define mutual inductance and self inductance. (A/M-15)

Transcription:

I²FG Workshop Impulse Forming May 7 th, 2013 Gent, Belgium Determination of suitable driver materials for electromagnetic sheet metal forming Soeren Gies

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 2 I 27

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 3 I 27

Introduction Objective: Electromagnetic forming of stainless steel 1.4301 and 1.4509 Challenge: Low electrical conductivity of stainless steel Copper Aluminum Steel Stainless steel CU-ETP CU-DHP EN AW-1050A EN AW-5083 DC06 1.4301 1.4509 57 MS/m 43 MS/m 34 MS/m 16 MS/m 8 MS/m 1.5 MS/m 100% 75% 60% 28% 14% 2,6% Solution: Use of driver sheets 4 I 27

Introduction Working principle of driver sheets: Upper tool (Forming die) t D t W Workpiece Driver sheet Coil winding Coil winding Lower tool (Flat working coil) Workpiece: 1.4301, t W = 0.8 mm Driver: Aluminum, t D =0.8 mm 5 I 27

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 6 I 27

Effect of driver sheets Use of driver sheets causes two opposing effects in the energy conversion sequence Ohmic heating Magnetic flux lines in the air Elastic energy in the die Energy supply Charging energy Coil energy Kinetic energy Forming energy Formingresult electromagnetic system (ƞ 1 ) mechanical system (ƞ 2 ) magn. pressure Energy conversion sequence: Risch, 2009 7 I 27

Effect of driver sheets Use of driver sheets causes two opposing effects in the energy conversion sequence Ohmic heating Magnetic flux lines in the air Elastic energy in the die Energy supply Charging energy Coil energy Kinetic energy Forming energy Forming energy driver sheet Formingresult electromagnetic system (ƞ 1 ) mechanical system (ƞ 2 ) magn. pressure Trade off: higher magnetic pressure vs. additional forming energy 8 I 27

Effect of driver sheets Use of driver sheets is beneficial if the following condition is fulfilled: Additional kinetic energy Additional forming energy for driver Optimum MAX Additional kinetic energy E kin Additional forming energy for driver E form Self-evident consequences: - High electrical conductivity E kin - Low yield strength E form Question: Which driver material and which driver thickness t D maximize the energy ratio? 9 I 27

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 10 I 27

State of the art Scientific investigations using driver sheets: Seth et al. (2004) Workpiece: Driver: Li et al. (2012) Workpiece: Driver: Low-alloy carbon steel, t W = 0.1 mm 0.38 mm Aluminium EN AW-6111 T4, t D = 1 mm Ti-6Al-4V, t W = 0.5 mm CU-DHP, t D = 0.5 mm Andersson and Syk (2008) Workpiece: Driver: Srinivasan et al. (2010) Workpiece: Driver: Ishibashi et al. (2011) Workpiece: Driver: X5CrNiMo17-12-2, t W = 0.25 mm / DP600, t W = 0.7 mm Copper, t D = 0.6 mm Titanium, t W = 0.076 mm Copper, t D = 0.381 mm X5CrNi18-10, t W = 0.15 mm EN AW-1050-H24, t D = 0.3 mm Workpiece thickness Driver thickness Skin depth 11 I 27

State of the art Scientific investigations using driver sheets: Tillmann et al. (2008) Workpiece: DC04, t W = 0,8 mm Driver: Copper (sputtered), t D = 0,65 mm (optimum) Recommendation: t D = σ s Bely et al. (1977) Recommendation: Desai et al. (2011) Workpiece: Driver: Recommendation: t D = 0,5 σ s Stainless steel Aluminum, Copper Aluminum t D = 0,8 σ s / Copper t D = σ s Contradicting recommendations No recommendation regarding optimal driver material No consideration of mechanical workpiece parameters Workpiece thickness Driver thickness Skin depth 12 I 27

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 13 I 27

Experimental Setup and Procedure 1 Free forming of workpiece and driver Upper tool (Drawing ring) Coil winding Lower tool (Flat coil) 100 mm 80 mm t D t W 65 mm 17 mm Pulse generator used: Maxwell Magneform 7000 Max. charging energy E C = 20 kj Short circuit frequency f* = 25 khz Inner resistance R i = 4.2 mω Inner inductance L i = 60 nh 14 I 27

Experimental Setup and Procedure 1 Free forming of workpiece and driver 2 Upper tool (Drawing ring) Coil winding 100 mm 80 mm t D t W Measuring of workpiece height h w h W Lower tool (Flat coil) 65 mm 17 mm Pulse generator used: Maxwell Magneform 7000 Max. charging energy E C = 20 kj Short circuit frequency f* = 25 khz Inner resistance R i = 4.2 mω Inner inductance L i = 60 nh h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D 15 I 27

Experimental Setup and Procedure Scope of investigations: Workpiece material 1.4301, t W = 0.5 / 0.8 / 1.0 mm 1.4509, t W = 0.5 / 0.8 / 1.0 mm DC04, t W = 0.5 / 0.8 / 1.0 mm EN AW-5083, t W = 1.0 mm Driver material CU-ETP, t D = 0.3 / 0.5 / 0.7 / 0.8 / 1.0 / 2.0 mm EN AW-1050A, t D = 0.3 / 0.5 / 0.7 / 0.8 / 1.0 / 2.0 mm Charging Energy E C E C = 1.0 / 1.8 / 2.4 kj 16 I 27

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 17 I 27

Results Workpiece: Material 1.4509 Thickness t W = 0.8 mm 100 mm 80 mm 24 17 mm 65 mm t D t W h W Forming height h w in mm 22 20 18 16 14 12 12 0 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Driver thickness t D Skin depthσ S 18 I 27

Results Workpiece: Material 1.4509 Thickness t W = 0.8 mm Optimum t D 1.05 σ S 100 mm 80 mm 24 17 mm 65 mm t D t W h W Forming height h w in mm 22 20 18 16 14 12 12 0 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Driver thickness t D Skin depthσ S 19 I 27

Results Workpiece: Material 1.4509 Thickness t W = 0.8 mm 100 mm 80 mm 17 mm 65 mm t D t W h W h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Forming height h w in mm 24 22 20 18 16 14 12 12 0 Optimum t D 1.05 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 Driver thickness t D Skin depthσ S E Form Driver Forming Energy E Kin Kinetic energy 20 I 27

Results Workpiece: Material 1.4509 Thickness t W = 0.8 mm 100 mm 80 mm 17 mm 65 mm t D t W h W h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Forming height h w in mm 24 22 20 18 16 14 12 12 0 Optimum t D 1.05 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 Driver thickness t D Skin depthσ S E Form Driver Forming Energy E Kin Kinetic energy 21 I 27

Results Workpiece: Material 1.4509 Thickness t W = 0.8 mm 100 mm 80 mm 17 mm 65 mm t D t W h W h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Forming height h w in mm 24 22 20 18 16 14 12 12 0 Driver AL CU Charging Energy E C 1.0 kj 1.8 kj 2.4 kj 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 Driver thickness t D Skin depthσ S 22 I 27

Results Workpiece: Material 1.4301 Thickness t W = 0.8 mm 100 mm 80 mm 17 mm 65 mm t D t W h W h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Forming height h w in mm 24 22 20 18 16 14 12 12 0 Driver AL CU Charging Energy E C 1.0 kj 1.8 kj 2.4 kj 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 Driver thickness t D Skin depthσ S 23 I 27

Results Workpiece: Material 1.4301 Thickness t W = 0.8 mm 100 mm 80 mm 17 mm 65 mm t D t W h W Forming height h w in mm Aluminium should be favoured 20 as driver material Optimum driver thickness t18 D,opt 1.1 σ s 1.2 σ s 24 22 16 14 12 12 0 Driver AL CU Conclusions Effect of charging energy E C because of varying strain Charging Energy E C 1.0 kj 1.8 kj 2.4 kj In case of very small strains (e.g. calibration) copper should be favoured 0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 h w = Workpiece forming height t w = Workpiece thickness = Driver thickness t D Driver thickness t D Skin depthσ S 24 I 27

Results Comparision of optimum driver thicknesses t D,opt (Driver material: AL) Workpiece thickness t W Workpiece material 0.5 mm 0.8 mm 1.0 mm 1.4301 0.95 σ s 1.0 σ s 1.27 σ s 1.4509 1.0 σ s 1.05 σ s 1.29 σ s Conclusions: Increasing workpiece thickness t W Increasing optimum driver thickness t D,opt Rule of thumb: Optimum driver thickness σ s (AL) 25 I 27

Agenda Introduction Effect of driver sheets State of the art Experimental setup and procedure Results Summary and Outlook 26 I 27

Summary and Outlook Summary: Aluminum should be favoured as driver material Positive correlation between workpiece thickness t W and optimum driver thickness t D,opt Rule of thumb: Optimum driver thickness σ s (AL) Outlook: EMF of stainless steel into a conical die using the optimum driver material und thickness Analytical calculation of the optimum driver thickness t D,opt 27 I 27

Questions? 28 I 27