MONTANA INSTRUMENTS MAGNET SOLUTIONS THIRD PARTY PRODUCT SOLUTIONS

Size: px
Start display at page:

Download "MONTANA INSTRUMENTS MAGNET SOLUTIONS THIRD PARTY PRODUCT SOLUTIONS"

Transcription

1 MONTANA INSTRUMENTS MAGNET SOLUTIONS THIRD PARTY PRODUCT SOLUTIONS GMW ASSOCIATES-5403 DIPOLE ELECTROMAGNET Adjustable pole gap 0-86mm Variety of pole tips 10mm, 38mm, & 76mm Air or water cooled Variety of mounting options PERFORMANCE OPTIONS Pole Face 10mm 38mm 76mm Pole Gap 2.5mm 3.44 T - 5.0mm 3.01 T - 7.5mm 2.66 T mm 2.35 T 2.18 T 1.62 T 19.0mm 1.61 T 1.24 T 25.4mm 1.31 T 1.07 T 38.1mm 0.92 T 0.84 T 50.8mm 0.69 T 0.69 T 76.2mm 0.43 T 0.49 T

2 THIRD PARTY PRODUCT SOLUTIONS ADVANTAGES OF GMW 5403 The GMW 5403 is capable of producing very high field strengths when integrated with a Montana Instruments System 1.6 Tesla at 20mm pole tip gap The range of pole tip gaps allow for large sample sizes of up to about 25 mm. The magnet design allows for a good uniformity of the magnetic field. Low working distances can be achieved. Many different pole face sizes are available and the pole tip gap of the magnet is adjustable. LIMITATIONS OF GMW 5403 The large size of the magnet coils can limit the size of the sample castle. Piezo selection and range of motion can be limited by the size and geometry of the sample castle. Magnet assembly is large and requires a substantial carriage for moving the magnet into position.

3 THIRD PARTY PRODUCT SOLUTIONS GMW ASSOCIATES-3470 AND 3480 DIPOLE ELECTROMAGNETS Adjustable pole gap 0-75mm Variety of pole tips 20mm and 40mm Air or water cooled Variety of mounting options PERFORMANCE OPTIONS POLE POLE GAP (mm) FACE (mm) MODEL T 1.1 T 0.8 T T 2.4 T 2.0 T 1.5 T 1.3 T 1.0 T 0.8 T 0.7 T 0.6 T T 1.0 T 0.7 T 0.6 T 0.5 T 0.4 T 0.4 T 0.4 T T 1.5 T 1.3 T 1.1 T 1.0 T 0.8 T 0.7 T 0.6 T 3480 GMW 3480 Field strength for 3470 magnet with various pole face sizes and pole tip gaps. Comparison between 3470 and 3480 magnets with 20mm pole faces at maximum amperage. GMW 3470

4 THIRD PARTY PRODUCT SOLUTIONS ADVANTAGES OF GMW 3480/3470 The GMW 3480 and 3470 are capable of producing very high field strengths when integrated with a Montana Instruments system. 1.0 Tesla with 3470 at 10mm pole tip gap 2.0 Tesla with 3480 at 10mm pole tip gap The range of pole tip gaps allow for large sample sizes of up to about 20 mm. The magnet assembly is smaller than the GMW 5403 Low working distances can be achieved. LIMITATIONS OF GMW 3480/3470 The size of the magnet coils can limit the size of the sample castle. Piezo selection and range of motion can be limited by the size and geometry of the sample castle. Magnet assembly requires a substantial carriage for moving the magnet into position. GMW 3470 GMW 3480

5 THIRD PARTY PRODUCT SOLUTIONS PERMANENT MAGNETS Permanent magnets can be an inexpensive and effective solution in certain applications. Consistent fields are provided and the magnet can be chosen to accomodate for different field strength requirements. Magnets can be mounted in vacuum housing recesses. Adjustable and custom mounting options are available (adjustable mount shown). Magnet Tube Vacuum Barrier Magnets (N52) Fits standard 50mm window port Adjust with 8mm Allen key (or by hand with large hex) Postion Adjustment Threaded portion translates magnets in to or out of the sample chamber

6 MONTANA INSTRUMENTS MAGNET SOLUTIONS ~1.31Tesla with 25.4 mm Pole Tip Spacing High field strength Low working distance ~3.6mm C2 Cryostation GMW5403 Dipole Electromagnet with 38mm pole faces (2x) Attocube ANPx311 positioners for sample positioning horizontally (1x) Attocube ANPz102 positioner for sample positioning vertically DIP16 electrical sample mount

7 MONTANA INSTRUMENTS MAGNET SOLUTIONS ~1.10 Tesla with 32 mm Pole Tip Spacing C2 Cryostation GMW5403 Dipole Electromagnet with 38mm pole faces Configuration 1: Sample mount post with mirror held at 45 for polar MOKE experiments Configuration 2: CB12 electrical sample mount for top and side LWD, (2x) Attocube ANPx311, (1x) Attocube ANPz102 CONFIGURATION 1 CONFIGURATION 2

8 MONTANA INSTRUMENTS MAGNET SOLUTIONS ~2.00 Tesla with 14 mm Pole Tip Spacing C2 Cryostation GMW5403 Dipole Electromagnet with 10mm pole faces Vertical and horizontal orientation of sample mount Coplanar waveguide PCB for Cryo-FMR experiments

9 ~0.40 Tesla with 35 mm Pole Tip Spacing C2 Cryostation GMW3470 Dipole Electromagnet with 40mm pole face (2x) Attocube ANPx101 and (1x) Attocube ANPz102 for sample motion

10 MONTANA INSTRUMENTS MAGNET SOLUTIONS PERMANENT MAGNET IN SAMPLE CHAMBER Nanoscale Workstation Horizontal Cryo-Optic Large motion on permanent magnet for varied field strength (2x) Attocube ANPx101 and (1x) Attocube ANPz102 for sample motion (3x) Attocube ANPx341 for magnet motion

11 Horizontal Cryo-Optic with Permanent Magnet NW2 Nanoscale Workstation Horizontal Cryo-Optic for imaging of sample (2x) Attocube ANPx101 positioners for sample positioning horizontally (1x) Attocube ANPz101 for sample positioning vertically Allows for permanent magnet access around the outside of the vacuum housing at various angles and locations TOP VIEW OF MAGNET ACCESS

Microscopy Cryostat System

Microscopy Cryostat System OF AMERICA, INC. Microscopy Cryostat System RC102-CFM Microscopy Cryostat offers fast cooldown, high efficiency, lowest thermal drift, excellent temperature stability and ultra low vibration Optical cryostat

More information

Transverse Field Profile of the NLC Damping Rings Electromagnet Wiggler

Transverse Field Profile of the NLC Damping Rings Electromagnet Wiggler LCC 0038 29/04/00 CBP Tech Note - 234 Linear Collider Collaboration Tech Notes Transverse Field Profile of the NLC Damping Rings Electromagnet Wiggler 29 April 2000 17 J. Corlett and S. Marks Lawrence

More information

Low Vibration Cryogenic Equipment

Low Vibration Cryogenic Equipment PAGE 12 PAGE 13 ATTOCUBE S CRYOSTATS ATTODRY attodry1000....................... 14 cryogen-free cryostats with/without s attodry700.........................18 cryogen-free table-top cryostats with optical

More information

Flanged Cryostats.

Flanged Cryostats. The liquid nitrogen cryostat is the most important and least appreciated component in assuring reliable long term performance of a germanium detector system. CANBERRA manufactures its own cryostats to

More information

A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU

A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU IWAA2004, CERN, Geneva, 4-7 October 2004 A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU D. P. Sanderson, NSCL-MSU, 1 Cyclotron Lab, East Lansing, MI 48824, USA 1. INTRODUCTION The Rare Isotope Accelerator

More information

Low Temperature Physics Measurement Systems

Low Temperature Physics Measurement Systems PAGE 6 & 2008 2007 PRODUCT CATALOG Accelerate your Semiconductor Research & Developments towards Nanoscale Products. Experience your new working horse in the emerging field of semiconductor research for

More information

Phys102 Lecture 16/17 Magnetic fields

Phys102 Lecture 16/17 Magnetic fields Phys102 Lecture 16/17 Magnetic fields Key Points Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on an Electric Charge Moving in a Magnetic

More information

Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences

Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences Outline Sample preparation Magnetron sputtering Ion-beam sputtering Pulsed laser deposition Electron-beam

More information

Magnetism. February 24, 2014 Physics for Scientists & Engineers 2, Chapter 27 1

Magnetism. February 24, 2014 Physics for Scientists & Engineers 2, Chapter 27 1 Magnetism February 24, 2014 Physics for Scientists & Engineers 2, Chapter 27 1 Magnetism! The Sun has massive magnetic fields as do other stars! The Earth also has a magnetic field! In the region of Magnesia,

More information

Analysis of Coupled Electromagnetic-Thermal Effects in Superconducting Accelerator Magnets

Analysis of Coupled Electromagnetic-Thermal Effects in Superconducting Accelerator Magnets Analysis of Coupled Electromagnetic-Thermal Effects in Superconducting Accelerator Magnets Egbert Fischer 1, Roman Kurnyshov 2 and Petr Shcherbakov 3 1 Gesellschaft fuer Schwerionenforschung mbh, Darmstadt,

More information

The Booster has three magnet systems for extraction: Kicker Ke, comprising two identical magnets and power supplies Septum Se

The Booster has three magnet systems for extraction: Kicker Ke, comprising two identical magnets and power supplies Septum Se 3.2.7 Booster Injection and Extraction 3.2.7.1 Overview The Booster has two magnet systems for injection: Septum Si Kicker Ki The Booster has three magnet systems for extraction: Kicker Ke, comprising

More information

Issues for Neutron Calculations for ITER Fusion Reactor

Issues for Neutron Calculations for ITER Fusion Reactor Introduction Issues for Neutron Calculations for ITER Fusion Reactor Erik Nonbøl and Bent Lauritzen Risø DTU, National Laboratory for Sustainable Energy Roskilde, Denmark Outline 1. Fusion development

More information

Chapter 27 Magnetism 1/20/ Magnets and Magnetic Fields Magnets and Magnetic Fields Magnets and Magnetic Fields

Chapter 27 Magnetism 1/20/ Magnets and Magnetic Fields Magnets and Magnetic Fields Magnets and Magnetic Fields Chapter 27 Magnetism Magnets have two ends poles called north and south. Like poles repel; unlike poles attract. However, if you cut a magnet in half, you don t get a north pole and a south pole you get

More information

VCE PHYSICS AOS 1 UNIT 4. Presented by Nick Howes

VCE PHYSICS AOS 1 UNIT 4. Presented by Nick Howes VCE PHYSICS AOS 1 UNIT 4 Presented by Nick Howes Forces on wires and DC Motors Key knowledge calculate magnitudes, including determining the directions of, and magnetic forces on, current carrying wires,

More information

3.2.2 Magnets. The properties of the quadrupoles, sextupoles and correctors are listed in tables t322_b,_c and _d.

3.2.2 Magnets. The properties of the quadrupoles, sextupoles and correctors are listed in tables t322_b,_c and _d. 3.2.2 Magnets The characteristics for the two types of combined function magnets,bd and BF, are listed in table t322_a. Their cross-sections are shown, together with the vacuum chamber, in Figure f322_a.

More information

Quantum Northwest, Inc. Product overview

Quantum Northwest, Inc. Product overview Quantum Northwest, Inc. Product overview February 2017 Offering the largest selection of Peltier-based cuvette holders on Earth. 1 Overview Quantum Northwest offers the largest selection of Peltier-based

More information

OASIS WIRELESS WEATHER STATION

OASIS WIRELESS WEATHER STATION User Manual 3910-B Royal Avenue, Simi Valley, Ca 93063 805-527-4498 RMIS Part No. 500760 TABLE OF CONTENTS INTRODUCTION General Description 3 General Precautions 3 INSTALLATION Base Preparation 6 Tower

More information

Switching of magnetic domains reveals spatially inhomogeneous superconductivity

Switching of magnetic domains reveals spatially inhomogeneous superconductivity Switching of magnetic domains reveals spatially inhomogeneous superconductivity Simon Gerber, Marek Bartkowiak, Jorge L. Gavilano, Eric Ressouche, Nikola Egetenmeyer, Christof Niedermayer, Andrea D. Bianchi,

More information

MAGNETS. Magnet types and performances Part 1

MAGNETS. Magnet types and performances Part 1 CERN Accelerator School Bruges, Belgium June 16-25, 2009 MAGNETS Magnet types and performances Part 1 Antoine DAËL CEA, Saclay, france CERN Accelerator School (CAS) Bruges, Belgium June 16-25, 2009 - Antoine

More information

Chapter 27 Magnetism. Copyright 2009 Pearson Education, Inc.

Chapter 27 Magnetism. Copyright 2009 Pearson Education, Inc. Chapter 27 Magnetism 27-1 Magnets and Magnetic Fields Magnets have two ends poles called north and south. Like poles repel; unlike poles attract. 27-1 Magnets and Magnetic Fields However, if you cut a

More information

Linear Collider Collaboration Tech Notes

Linear Collider Collaboration Tech Notes LCC 0035 07/01/00 Linear Collider Collaboration Tech Notes More Options for the NLC Bunch Compressors January 7, 2000 Paul Emma Stanford Linear Accelerator Center Stanford, CA Abstract: The present bunch

More information

CHAPTER 20 Magnetism

CHAPTER 20 Magnetism CHAPTER 20 Magnetism Units Magnets and Magnetic Fields Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on Electric Charge Moving in a Magnetic

More information

Assembly Instructions for the 1-Wire Weather Station V2.0/V3.0

Assembly Instructions for the 1-Wire Weather Station V2.0/V3.0 Assembly Instructions for the 1-Wire Weather Station V2.0/V3.0 Tools and Supplies Required (not included): Phillips screwdriver 3/8" wrench Drill with 5/32" bit "U" type mounting bracket (i.e., part number

More information

Atomic Force/Magnetic Force Microscope

Atomic Force/Magnetic Force Microscope Atomic Force/Magnetic Force Microscope Veeco Instruments Dimension 3000 SPM with Nanoscope IIIa controller Atomic Force Microscopy Mode Magnetic Force Microscopy Mode Vibration isolation and sound proof

More information

Electron charge-to-mass ratio

Electron charge-to-mass ratio (ta initials) first name (print) last name (print) brock id (ab17cd) (lab date) Experiment 4 Electron charge-to-mass ratio In this Experiment you will learn the relationship between electric and magnetic

More information

Magnetic Fields

Magnetic Fields Magnetic circuits introduction Becomes aware of the similarities between the analysis of magnetic circuits and electric circuits. Develop a clear understanding of the important parameters of a magnetic

More information

Status of the MAGIX Spectrometer Design. Julian Müller MAGIX collaboration meeting 2017

Status of the MAGIX Spectrometer Design. Julian Müller MAGIX collaboration meeting 2017 Status of the MAGIX Spectrometer Design Julian Müller MAGIX collaboration meeting 2017 Magneto Optic Design Requirements relative momentum resolution Δp p < 10 4 resolution of the scattering angle Δθ

More information

224 g (Total 1 mark) A straight line in a direction opposite to that of the field.

224 g (Total 1 mark) A straight line in a direction opposite to that of the field. Q1. The diagram shows a rigidly-clamped straight horizontal current-carrying wire held mid-way between the poles of a magnet on a top pan balance. The wire is perpendicular to the magnetic field direction.

More information

Chapter 21. Magnetic Forces and Magnetic Fields

Chapter 21. Magnetic Forces and Magnetic Fields Chapter 21 Magnetic Forces and Magnetic Fields 1 21.1 Magnetic Fields The phenomenon of magnetism (1) The magnetic compass In Class Demo The needle of a compass is a permanent magnet that has a north magnetic

More information

A Technical Proposal for the Development and Manufacturing of Electromagnets for the TESLA Beam Delivery System

A Technical Proposal for the Development and Manufacturing of Electromagnets for the TESLA Beam Delivery System D.V. Efremov Scientific Research Institute of Electrophysical Apparatus Scientific Technical Center SINTEZ Scientific Technical Center TEMP A Technical Proposal for the Development and Manufacturing of

More information

Magnetic Engines For Low Orbit Leading to Development of Deep Space Transport. By Jerry L. Decker A Retired Engineer. Abstract

Magnetic Engines For Low Orbit Leading to Development of Deep Space Transport. By Jerry L. Decker A Retired Engineer. Abstract Magnetic Engines For Low Orbit Leading to Development of Deep Space Transport By Jerry L. Decker A Retired Engineer Abstract Magnetic engines are proposed for saving energy in surface to orbit launches

More information

Magnet Buildability Review report : C-Beta Magnets

Magnet Buildability Review report : C-Beta Magnets Magnet Buildability Review report : C-Beta Magnets Date: December 16 th, 2016 Reviewers: T. Tanabe (chair), M. Anerella, M. Harrison, A. Temnykh and J. Tuozzolo Participants: S. Peggs, K. Smolenski, G.

More information

Extraction from cyclotrons. P. Heikkinen

Extraction from cyclotrons. P. Heikkinen Extraction from cyclotrons P. Heikkinen Classification of extraction schemes Linear accelerators Circular accelerators No extraction problem Constant orbit radius (sychrotrons, betatrons) Increasing orbit

More information

Lattice Cell/Girder Assembly

Lattice Cell/Girder Assembly SPEAR3 Magnets Jack Tanabe, Nanyang Li, Ann Trautwein, Domenico Dell Orco, Dave Ernst, Zach Wolf (SLAC Magnet Measurements), Catherine L Coq (SLAC Alignment), Jeff Corbett, Bob Hettel (SPEAR3 Physics)

More information

INSTITUTE FOR TECHNICAL PHYSICS (ITEP) CRYOGENICS

INSTITUTE FOR TECHNICAL PHYSICS (ITEP) CRYOGENICS Design and Construction of the Cryogenic Cooling System for the Rotating Magnetic Validator of the 10 MW SUPRAPOWER Offshore Superconducting Wind Turbine Jiuce Sun, Holger Neumann, Santiago Sanz, Gustavo

More information

Impact of the forces due to CLIQ discharges on the MQXF Beam Screen. Marco Morrone, Cedric Garion TE-VSC-DLM

Impact of the forces due to CLIQ discharges on the MQXF Beam Screen. Marco Morrone, Cedric Garion TE-VSC-DLM Impact of the forces due to CLIQ discharges on the MQXF Beam Screen Marco Morrone, Cedric Garion TE-VSC-DLM The High Luminosity - LHC project HL-LHC Beam screen design - Beam screen dimensions - Conceptual

More information

EE 410/510: Electromechanical Systems Chapter 4

EE 410/510: Electromechanical Systems Chapter 4 EE 410/510: Electromechanical Systems Chapter 4 Chapter 4. Direct Current Electric Machines and Motion Devices Permanent Magnet DC Electric Machines Radial Topology Simulation and Experimental Studies

More information

Physics 54 Lecture March 1, Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields

Physics 54 Lecture March 1, Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields Physics 54 Lecture March 1, 2012 OUTLINE Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields Electromagnetic induction Introduction to electromagnetic

More information

CRYOGENIC SYSTEMS FOR INERTIAL FUSION ENERGY. CEA-Grenoble France DSM/DRFMC/SBT

CRYOGENIC SYSTEMS FOR INERTIAL FUSION ENERGY. CEA-Grenoble France DSM/DRFMC/SBT CRYOGENIC SYSTEMS FOR INERTIAL FUSION ENERGY CEA-Grenoble France DSM/DRFMC/SBT D.Chatain JP. Périn, P.Bonnay, E.Bouleau, M.Chichoux, D.Communal, J.Manzagol, F.Viargues, D.Brisset, G. Paquignon, V.Lamaison.

More information

PHYSICS Fall Lecture 15. Electromagnetic Induction and Faraday s Law

PHYSICS Fall Lecture 15. Electromagnetic Induction and Faraday s Law PHYSICS 1444-001 Fall 2012 Lecture 15 Electromagnetic Induction and Faraday s Law A current can be produced by a changing magnetic field First shown in an experiment by Michael Faraday Induced emf A primary

More information

-magnetic dipoles are largely analogous to electric dipole moments -both types of dipoles

-magnetic dipoles are largely analogous to electric dipole moments -both types of dipoles Student Name Date Manipulating Magnetization Electric dipole moment: Magnetic dipole moment: -magnetic dipoles are largely analogous to electric dipole moments -both types of dipoles -physical separation

More information

Development of superconducting undulators at the Advanced Photon Source

Development of superconducting undulators at the Advanced Photon Source Development of superconducting undulators at the Advanced Photon Source Presented by Vadim Sajaev on behalf of the APS superconducting undulator project team Advanced Photon Source Argonne National Laboratory

More information

1 Solution of Electrostatics Problems with COM- SOL

1 Solution of Electrostatics Problems with COM- SOL 1 Solution of Electrostatics Problems with COM- SOL This section gives examples demonstrating how Comsol can be used to solve some simple electrostatics problems. 1.1 Laplace s Equation We start with a

More information

AXTRUSION SUPPLEMENTARY MATERIALS. An approximate formula for estimating a bearing s stiffness is 1. P s A 2 h

AXTRUSION SUPPLEMENTARY MATERIALS. An approximate formula for estimating a bearing s stiffness is 1. P s A 2 h Appendix A AXTRUSION SUPPLEMENTARY MATERIALS A. Carriage Stiffness Estimates This section describes the steps to predict the stiffness performance of the carriage. First an accurate stiffness model of

More information

Optical Microscopy Study of Topological Insulators Using Ellipsometry

Optical Microscopy Study of Topological Insulators Using Ellipsometry Optical Microscopy Study of Topological Insulators Using Ellipsometry Amber Schedlbauer August 23, 2011 1 Abstract An optical setup based on normal-incidence reflectivity allows the Magneto Optic Kerr

More information

ORMS HARS. SpectrA LAB EQUIPMENTS Optical Rotation Resolution nm Wavelength Range 0.1nm Wavelength Resolution -70 C Cooling 10 Vacuum

ORMS HARS. SpectrA LAB EQUIPMENTS Optical Rotation Resolution nm Wavelength Range 0.1nm Wavelength Resolution -70 C Cooling 10 Vacuum All Products are manufactured and marketed by Opto-Mechatronics Pvt. Ltd HARS ADVANCED RESEARCH SYSTEMS & SOLUTIONS FARADAY & KERR OPTO-MECHATRONICS PVT.LTD OPTICAL ROTATION MEASUREMENT SYSTEM 0-3 0.005

More information

Class 11 : Magnetic materials

Class 11 : Magnetic materials Class 11 : Magnetic materials Magnetic dipoles Magnetization of a medium, and how it modifies magnetic field Magnetic intensity How does an electromagnet work? Boundary conditions for B Recap (1) Electric

More information

SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM]

SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM] G01Q SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM] Scanning probes, i.e. devices having at least a tip of nanometre sized dimensions

More information

A little history. Electricity and Magnetism are related!

A little history. Electricity and Magnetism are related! Intro to Magnetism A little history Until the early 19 th century, scientists thought electricity and magnetism were unrelated In 1820, Danish science professor Hans Christian Oersted was demonstrating

More information

Experiment Ma8: Superconductivity

Experiment Ma8: Superconductivity Experiment Ma8: Superconductivity 1 Overview Superconductivity is a phenomenon occurring at low temperatures. H.K. Onnes observed in year 1911 that the electrical resistivity of some metals sank abruptly

More information

Testing and Final Construction of the Superconducting Magnet for the Alpha Magnetic Spectrometer

Testing and Final Construction of the Superconducting Magnet for the Alpha Magnetic Spectrometer Testing and Final Construction of the Superconducting Magnet for the Alpha Magnetic Spectrometer The MIT Faculty has made this article openly available. Please share how this access benefits you. Your

More information

SpRIT TPC: Device to constrain the symmetry energy at supra-saturation densities

SpRIT TPC: Device to constrain the symmetry energy at supra-saturation densities SpRIT TPC: Device to constrain the symmetry energy at supra-saturation densities Jonathan Barney for SpRIT TPC Collaboration 4/17/2015 Outline Motivation: Probing the EoS at suprasaturation densities 2

More information

Lab 8: Magnetic Fields

Lab 8: Magnetic Fields Lab 8: Magnetic Fields Name: Group Members: Date: TA s Name: Objectives: To measure and understand the magnetic field of a bar magnet. To measure and understand the magnetic field of an electromagnet,

More information

Electromagnetism 2. D. the charge moves at right angles to the lines of the magnetic field. (1)

Electromagnetism 2. D. the charge moves at right angles to the lines of the magnetic field. (1) ame: Date: Electromagnetism 2 1. A magnetic force acts on an electric charge in a magnetic field when A. the charge is not moving. B. the charge moves in the direction of the magnetic field. C. the charge

More information

Accelerators. Table Quadrupole magnet

Accelerators. Table Quadrupole magnet Accelerators 2.6 Magnet System 2.6.1 Introduction According to the BEPCII double ring design scheme, a new storage ring will be added in the existing BEPC tunnel. The tasks of the magnet system can be

More information

Design of a Dipole with Longitudinally Variable Field using Permanent Magnets for CLIC DRs

Design of a Dipole with Longitudinally Variable Field using Permanent Magnets for CLIC DRs Design of a Dipole with Longitudinally Variable Field using Permanent Magnets for CLIC DRs M. A. Domínguez, F. Toral (CIEMAT), H. Ghasem, P. S. Papadopoulou, Y. Papaphilippou (CERN) Index 1. Introduction

More information

Lecture Notes ELEC A6

Lecture Notes ELEC A6 Lecture Notes ELEC A6 Dr. Ramadan El-Shatshat Magnetic circuit 9/27/2006 Elec-A6 - Electromagnetic Energy Conversion 1 Magnetic Field Concepts Magnetic Fields: Magnetic fields are the fundamental mechanism

More information

Chapter 27 Magnetism. Copyright 2009 Pearson Education, Inc.

Chapter 27 Magnetism. Copyright 2009 Pearson Education, Inc. Chapter 27 Magnetism 27-1 Magnets and Magnetic Fields Magnets have two ends poles called north and south. Like poles repel; unlike poles attract. 27-1 Magnets and Magnetic Fields However, if you cut a

More information

MAGNETIC FIELDS CHAPTER 21

MAGNETIC FIELDS CHAPTER 21 MAGNETIC FIELDS CHAPTER 21 1. A magnetic field may exist at a point as a result of moving charged particle 2. When a tiny bar magnet is suspended horizontally from its center, it lines up along the north

More information

Revision 1.0, January 2014 MICRONIX USA, LLC

Revision 1.0, January 2014 MICRONIX USA, LLC 2014 Edition Revision 1.0, January 2014 MICRONIX USA, LLC The information within regarding the MICRONIX USA Product Line and/or any other products and technology owned by MICRONIX USA, LLC are subject

More information

QUESTION 1. Answer: N

QUESTION 1. Answer: N MAGNETISM Review QUESTION 1 A proton speeding through a synchrotron at 3.0 10 7 m/s experiences a magnetic field of 3.0 T that is produced by the steering magnets in the synchrotron. What is the magnetic

More information

PHY3901 PHY3905. Hall effect and semiconductors Laboratory protocol

PHY3901 PHY3905. Hall effect and semiconductors Laboratory protocol PHY3901 PHY3905 Hall effect and semiconductors Laboratory protocol PHY3901 PHY3905 Hall effect and semiconductors Laboratory protocol Objectives Observe and qualitatively understand the phenomenon of transverse

More information

Addition 1. Shear Stack Piezoelectric Elements and Shear Effect Basics

Addition 1. Shear Stack Piezoelectric Elements and Shear Effect Basics 120 Addition 1 Shear Stack Piezoelectric Elements and Shear Effect Basics Introduction The STM scanner built up in this work is a Besocke type scanner (see room temperature STM instrumental chapter). The

More information

The SOS Quad in the Right-HRS (RHRS)

The SOS Quad in the Right-HRS (RHRS) The SOS Quad in the Right-HRS (RHRS) Barak Schmookler Apex- Apr. 19, 2015 1 Current Status of the RHRS The HRSs (RHRS and LHRS) are QQDQ spectrometers. Quadrupole 1 (Q1) focuses in the dispersive (i.e.

More information

ICSE Board Class IX Physics Paper 5

ICSE Board Class IX Physics Paper 5 ICSE Board Class IX Physics Paper 5 Time: 2 hrs Total Marks: 80 General Instructions: 1. Answers to this paper must be written on the paper provided separately. 2. You will not be allowed to write during

More information

GEODETIC MEASUREMENTS FOR THE HERA PROTON RING, THE NEW EXPERIMENTS AND THE TESLA TEST FACILITY - A STATUS REPORT

GEODETIC MEASUREMENTS FOR THE HERA PROTON RING, THE NEW EXPERIMENTS AND THE TESLA TEST FACILITY - A STATUS REPORT I/1 GEODETIC MEASUREMENTS FOR THE HERA PROTON RING, THE NEW EXPERIMENTS AND THE TESLA TEST FACILITY - A STATUS REPORT F. Löffler, DESY Hamburg Abstract The HERA proton machine has been operating since

More information

Speed of Light in Air

Speed of Light in Air Speed of Light in Air Electromagnetic waves represent energy in the form of oscillating electric and magnetic fields which propagate through vacuum with a speed c = 2.9979246x10 8 m/s. Electromagnetic

More information

CH 19-1 Magnetic Field

CH 19-1 Magnetic Field CH 19-1 Magnetic Field Important Ideas A moving charged particle creates a magnetic field everywhere in space around it. If the particle has a velocity v, then the magnetic field at this instant is tangent

More information

Kirchhoff s rules, example

Kirchhoff s rules, example Kirchhoff s rules, example Magnets and Magnetism Poles of a magnet are the ends where objects are most strongly attracted. Two poles, called north and south Like poles repel each other and unlike poles

More information

Magnetism II. Physics 2415 Lecture 15. Michael Fowler, UVa

Magnetism II. Physics 2415 Lecture 15. Michael Fowler, UVa Magnetism II Physics 2415 Lecture 15 Michael Fowler, UVa Today s Topics Force on a charged particle moving in a magnetic field Path of a charged particle moving in a magnetic field Torque on a current

More information

INTRODUCTION to the DESIGN and FABRICATION of IRON- DOMINATED ACCELERATOR MAGNETS

INTRODUCTION to the DESIGN and FABRICATION of IRON- DOMINATED ACCELERATOR MAGNETS INTRODUCTION to the DESIGN and FABRICATION of IRON- DOMINATED ACCELERATOR MAGNETS Cherrill Spencer, Magnet Engineer SLAC National Accelerator Laboratory Menlo Park, California, USA Lecture # 1 of 2 Mexican

More information

Chapter 21. Magnetic Forces and Magnetic Fields

Chapter 21. Magnetic Forces and Magnetic Fields Chapter 21 Magnetic Forces and Magnetic Fields 21.1 Magnetic Fields The needle of a compass is permanent magnet that has a north magnetic pole (N) at one end and a south magnetic pole (S) at the other.

More information

[ Extract from Astronomical Spectroscopy for Amateurs ] 18.0 Guiding, OAG and Beam splitters/ Flip mirrors Off Axis Guiders

[ Extract from Astronomical Spectroscopy for Amateurs ] 18.0 Guiding, OAG and Beam splitters/ Flip mirrors Off Axis Guiders [ Extract from Astronomical Spectroscopy for Amateurs ] 18.0 Guiding, OAG and Beam splitters/ Flip mirrors You ll quickly find it s a challenge to get a star focused on the spectroscope slit and hold it

More information

Detection of Wear in Oilwell Service Tubings using Magnetic Flux Leakage

Detection of Wear in Oilwell Service Tubings using Magnetic Flux Leakage Detection of Wear in Oilwell Service Tubings using Magnetic Flux Leakage Many methods have been developed and used for the inspection of oilwell service tubings to find wear, corrosion and fractures. One

More information

Insertion Devices Lecture 6 The Application of Superconductors. Jim Clarke ASTeC Daresbury Laboratory

Insertion Devices Lecture 6 The Application of Superconductors. Jim Clarke ASTeC Daresbury Laboratory Insertion Devices Lecture 6 The Application of Superconductors Jim Clarke ASTeC Daresbury Laboratory Introduction For fields greater than ~3T superconductors are the only real option For intermediate fields

More information

SpRIT TPC: Device to constrain the symmetry energy at supra-saturation densities

SpRIT TPC: Device to constrain the symmetry energy at supra-saturation densities SpRIT TPC: Device to constrain the symmetry energy at supra-saturation densities Jonathan Barney for SpRIT TPC Collaboration 1/11/2016 Outline Motivation: Probing the EoS at suprasaturation densities 2

More information

Polarized 3 He Target For Future Experiments

Polarized 3 He Target For Future Experiments Polarized 3 He Target For Future Experiments Kai Jin, University of Virginia, on behalf of JLab polarized 3 He group Hall C Winter Collaboration Meeting, January 20, 2017 Introduction to polarized 3 He

More information

AMOR the time-of-flight neutron reflectometer at SINQ/PSI

AMOR the time-of-flight neutron reflectometer at SINQ/PSI PRAMANA c Indian Academy of Sciences Vol. 63, No. 1 journal of July 2004 physics pp. 57 63 AMOR the time-of-flight neutron reflectometer at SINQ/PSI MUKUL GUPTA 1, T GUTBERLET 1, J STAHN 1, P KELLER 1

More information

Current in a Magnetic Field Learning Outcomes. Force on a Current-Carrying Conductor

Current in a Magnetic Field Learning Outcomes. Force on a Current-Carrying Conductor 1 Current in a Magnetic Field Learning Outcomes Discuss the force on a current-carrying conductor in a magnetic field. Demonstrate this force. Solve problems about this force. Discuss applications of this

More information

Physics 010 Midterm #2

Physics 010 Midterm #2 Physics 010 Midterm #2 Thursday April 2, 8:30 10:00am This midterm is closed book. No books or notes allowed. Calculators are allowed There are 10 questions on this midterm, with marks noted beside each

More information

The ZEPTO project: Tuneable permanent magnets for the next generation of high energy accelerators.

The ZEPTO project: Tuneable permanent magnets for the next generation of high energy accelerators. The ZEPTO project: Tuneable permanent magnets for the next generation of high energy accelerators. Alex Bainbridge, Ben Shepherd, Norbert Collomb, Jim Clarke. STFC Daresbury Laboratory, UK Michele Modena,

More information

Cambridge International Examinations Cambridge International General Certificate of Secondary Education (9 1)

Cambridge International Examinations Cambridge International General Certificate of Secondary Education (9 1) Cambridge International Examinations Cambridge International General Certificate of Secondary Education (9 1) *0123456789* PHYSICS 0972/03 Paper 3 Theory (Core) For Examination from 2018 SPECIMEN PAPER

More information

Development of a Compressor for a Miniature Pulse Tube Cryocooler of 2.5 W at 65 K

Development of a Compressor for a Miniature Pulse Tube Cryocooler of 2.5 W at 65 K Development of a Compressor for a Miniature Pulse Tube Cryocooler of 2.5 W at 65 K N. Matsumoto, Y. Yasukawa, K. Ohshima, T. Takeuchi, K. Yoshizawa, T. Matsushita, Y. Mizoguchi, and A. Ikura Fuji Electric

More information

Chapter 21. Magnetism

Chapter 21. Magnetism Chapter 21 Magnetism Magnets Poles of a magnet are the ends where objects are most strongly attracted Two poles, called north and south Like poles repel each other and unlike poles attract each other Similar

More information

Physics H. Instructor: Dr. Alaa Mahmoud

Physics H. Instructor: Dr. Alaa Mahmoud Physics 202 1436-1437 H Instructor: Dr. Alaa Mahmoud E-mail: alaa_y_emam@hotmail.com Chapter 28 magnetic Field Magnetic fingerprinting allows fingerprints to be seen on surfaces that otherwise would not

More information

Free electron lasers

Free electron lasers Preparation of the concerned sectors for educational and R&D activities related to the Hungarian ELI project Free electron lasers Lecture 2.: Insertion devices Zoltán Tibai János Hebling 1 Outline Introduction

More information

Vacuum Kelvin Force Probe Research Richard Williams August 1st 2008

Vacuum Kelvin Force Probe Research Richard Williams August 1st 2008 Vacuum Kelvin Force Probe Research Richard Williams August 1st 2008 Introduction Kelvin Force Probe Microscopy is an analytical method to measure the contact potential difference between a reference material

More information

1. Introduction. 2. Concept

1. Introduction. 2. Concept SLAC-PUB-11412 FINDING THE MAGNETIC CENTER OF A QUADRUPOLE TO HIGH RESOLUTION G. E. Fischer, J. K. Cobb, D. R. Jenson Stanford Linear Accelerator Center Stanford, CA. 1. Introduction In a companion proposal

More information

SCS 139 Applied Physics II

SCS 139 Applied Physics II SCS 139 Applied Physics II Dr. Prapun Suksompong prapun@siit.tu.ac.th www.prapun.com Office Hours: BKD 3601-7 Monday 9:20-10:20 Wednesday 9:20-10:20 1 i Course Web Site Please check the course website

More information

Review of proposals of ERL injector cryomodules. S. Belomestnykh

Review of proposals of ERL injector cryomodules. S. Belomestnykh Review of proposals of ERL injector cryomodules S. Belomestnykh ERL 2005 JLab, March 22, 2005 Introduction In this presentation we will review injector cryomodule designs either already existing or under

More information

Quick Start Guide. The ieq45 GoTo German Equatorial Mount # 8000C

Quick Start Guide. The ieq45 GoTo German Equatorial Mount # 8000C Quick Start Guide The ieq45 GoTo German Equatorial Mount # 8000C PACKAGE CONTENTS Telescope Mount (with built-in GPS) 3.5 Vixen type dovetail saddle (installed on the mount) 8 Losmandy-D type dovetail

More information

Magnetic Forces and Magnetic Fields

Magnetic Forces and Magnetic Fields Magnetic Forces and Magnetic Fields 21.1 Magnetic Fields The behavior of magnetic poles is similar to that of like and unlike electric charges. 21.1 Magnetic Fields The needle of a compass is permanent

More information

The SIS100 Superconducting Magnets

The SIS100 Superconducting Magnets The SIS100 Superconducting Magnets Anna Mierau Workshop Beam physics for FAIR 2012 May 10 11, 2012 Hotel Haus Schönblick 1. Overview of superconducting beam guiding magnets of the SIS100 - Requirements

More information

TAP 416-3: Alternating current generators

TAP 416-3: Alternating current generators TAP 416-3: Alternating current generators Thinking about generators and induced emf An emf is induced in a coil when the magnetic flux through the coil changes. The emf in volts is numerically equal to

More information

CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD

CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD K. Nam, a D. K. Kang, a W. Chung, a C. H. Noh, a J. Yu, b N. I. Her, b C. Hamlyn-Harris, b Y. Utin, b and K.

More information

30 MM CAGE CUBE-MOUNTED CIRCULAR POLARIZERS

30 MM CAGE CUBE-MOUNTED CIRCULAR POLARIZERS 30 MM CAGE CUBE-MOUNTED CIRCULAR POLARIZERS Creates Circularly Polarized Output from Arbitrarily Polarized Input 30 mm Cage Cube Housing Wave Plate can be Rotated to Output Linear or Elliptical Polarization

More information

OPTICAL PARTICLE SIZER MASS CALIBRATION METHOD

OPTICAL PARTICLE SIZER MASS CALIBRATION METHOD OPTICAL PARTICLE SIZER MASS CALIBRATION METHOD APPLICATION NOTE OPS-001 The Optical Particle Sizer (OPS) is calibrated for size with Polystyrene Latex (PSL) spheres (per ISO 12501-1/4) at TSI. This method

More information

INPAQ. Specification. WIP252012S L Series. Product Name. Power Inductor. Size EIAJ Global RF/Component Solutions

INPAQ. Specification. WIP252012S L Series. Product Name. Power Inductor. Size EIAJ Global RF/Component Solutions WIP252012S L Series Specification Product Name Series Power Inductor WIP252012S L Series Size EIAJ 2520 WIP252012S L Series Engineering Specification 1. Scope Feature High saturation current realized by

More information

The PEP-I1 B-Factory Septum Quadrupole Magnet

The PEP-I1 B-Factory Septum Quadrupole Magnet Y The PEP-I1 B-Factory Septum Quadrupole Magnet Johanna M Swan, Arthur R Harvey, Robert H Holmes, C Matthew Kendall, Robert M Yamamoto, and Ted T Yokota (LLNL) Jack T Tanabe and Ross D Schlueter (LBL)

More information

Magnetic Fields and Forces

Magnetic Fields and Forces Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 20 Magnetic Fields and Forces Marilyn Akins, PhD Broome Community College Magnetism Magnetic fields are produced by moving electric charges

More information