Force acting on a charged particle moving through a magnetic field

Slides:



Advertisements
Similar presentations
Magnetic Force on a Current-Carrying Conductor
Advertisements

 When a current moves through a conductor in a magnetic field a force is produced.  Michael Faraday discovered that the force on the wire is at right.
Electricity and Magnetism
The Magnetic Force Between Two Parallel Conductors AP Physics C Montwood High School R. Casao.
THE MAGNETIC FORCE BETWEEN TWO PARALLEL CONDUCTORS Lecture No.12 By. Sajid Hussain Qazi.
Lecture 7 Magnetic Field and Magnetic Force Chapter 19.1  19.6 Outline Magnets Magnetic Field Magnetic Force Motion in a Magnetic Field.
Example: A negatively charged rod, of length l, has a total charge Q and is a distance b from a point P. The charge is uniformly distributed along the.
With permanent magnets opposite poles attract and like poles repel. As we have seen magnetic fields surround any current carrying wire. Therefore it stands.
1 Chapter Flux Number of objects passing through a surface.
Measuring the strength of a Magnetic Field © David Hoult 2009.
Topic 12.1 Induced electromotive force (emf) 3 hours.
Hall Effect. E and B  Charged particles can be subject to both electric and magnetic fields.
The Magnetic Field The force on a charge q moving with a velocity The magnitude of the force.
Magnetism Magnetic Force 1 Magnetic Force on a Moving Charge Magnetic Force on a Current Carrying Wire.
The Magnetic Field The force on a charge q moving with a velocity The magnitude of the force.
Electricity and Magnetism: Electromagnets Mr D. Patterson.
Magnetism Magnetic Force. Magnetic Force Outline Lorentz Force Charged particles in a crossed field Hall Effect Circulating charged particles Motors Bio-Savart.
Physics of Fusion power Lecture4 : Quasi-neutrality Force on the plasma.
Flux Density due to a current flowing in a long straight wire © David Hoult 2009.
Magnetic Fields Magnetic fields emerge from the North pole of a magnet and go into the South pole. The direction of the field lines show the direction.
Chapter 22 Gauss’s Law. Charles Allison © Motion of a Charged Particle in an Electric Field The force on an object of charge q in an electric.
A basic property of the tiny particles that make up matter; it can be positive or negative: Some particles of matter have an electric charge. Electric.
Starting with …. BE (TELECOM) IV What is current ? current is a flow of electric charge What is density ? Density is a property of matter that is unique.
Electromagnetism Loop - the questions will cycle so you will see them again! 1. Caused by having more electrons than protons (negative) or more protons.
Electro-Magnetism © David Hoult Magnetic Field Shapes © David Hoult 2009.
MAGNETISM MAMBO.
6.3.6 Solve problems involving magnetic forces, fields and currents.
Magnetism 1. 2 Magnetic fields can be caused in three different ways 1. A moving electrical charge such as a wire with current flowing in it 2. By electrons.
Copyright © 2009 Pearson Education, Inc. Lecture 4 – Electricity & Magnetism (Electrostatics) a. Electric Charge, Electric Field & Gauss’ Law.
Faraday’s Law: Generalized A loop moving in a field has a current induced (Think F=qvB) If the loop is stationary, and the magnet moves, a current is still.
Magnetic Field Strength and Magnetic Force O An electrically charged particle moving in a magnetic field may experience a magnetic force. O Magnetic Field.
Lectures 11 & 12: Magnetic Fields and the Motion of Charged Particles Chapters (Tipler) Electro magnetism.
Magnetic Fields Chapter The force exerted by a magnetic field Definition of B 26.3 Motion of a charged particle in a magnetic field Applications.
Magnetism and magnetic forces. Current off coil Molecular magnets aligned randomly N S.
Electromagnetism Lecture#15 Instructor: Muhammad Mateen Yaqoob.
Electromagnetism Topic 12.1 Electromagnetic Induction.
Magnetic Fields. MAGNETOSTATICS Magnetic Fields Fundamental Postulates of Magnetostatics in Free Space.
Magnetic Fields. Magnetic Fields and Forces a single magnetic pole has never been isolated magnetic poles are always found in pairs Earth itself is a.
Electricity and Magnetism
Week 9 Presentation 1 Electromagnets 1. Learning Objectives: 1. Determine the magnitude and direction of the magnetic field strength generated by a straight.
Magnetic Fields Starter questions
Current in a Magnetic Field – Learning Outcomes 1.
12: Electromagnetic Induction
2.2 ELECTROMAGNETISM 19th November 2012
Chapter five conduction
Magnetic Forces on Wires and Charges
Magnetism Magnetism Lecture 15 Today Magnetic Fields
Electric Flux & Gauss Law
Lecture 01: Electric Fields & Forces
Electricity and Magnetism
Hall Effect When a current carrying conductor is placed in a magnetic field, a potential difference is generated in a direction perpendicular to both the.
Electro-Magnetic Induction
Electricity and Magnetism
Current in a Magnetic Field
+.
The Effect Of A Magnetic Field On Charged Particles
Let’s look in detail at each of these four ways of using flux change or motion to produce an emf. Method 3…
Topic 12.1 Electromagnetic Induction
Flux density produced by a long coil (solenoid)
Magnetic Fields Chapter 26 Definition of B
Today’s agenda: Induced emf. Faraday’s Law. Lenz’s Law. Generators.
Measuring the strength of a Magnetic Field
Electricity and Magnetism
5. Magnetic forces on current
Magnetic Fields and Magnetic Force
Force acting between two long, parallel, current-carrying conductors
Moving Charges In Magnetic and Electric Fields
The Motion of Charged Particles in Magnetic Fields
Just like the ’Motor effect’ – a charged particle experiences a force when Moving through a magnetic field – Use the Slap Rule (thumb is v) F=Bqv.
Stationary Magnetic field
Presentation transcript:

Force acting on a charged particle moving through a magnetic field © D Hoult 2008

Consider a conductor of length L, having n free electrons per unit volume. A current, I is flowing through it

Consider a conductor of length L, having n free electrons per unit volume. A current, I is flowing through it

In this piece of conductor there are

In this piece of conductor there are NAL free electrons

In this piece of conductor there are NAL free electrons If all these electrons pass through end x in time t then the current, I is given by

In this piece of conductor there are NAL free electrons If all these electrons pass through end x in time t then the current, I is given by n A L e t

If there is a magnetic field of flux density B at 90° to the current, the conductor will experience a force of magnitude

If there is a magnetic field of flux density B at 90° to the current, the conductor will experience a force of magnitude I L B

If there is a magnetic field of flux density B at 90° to the current, the conductor will experience a force of magnitude I L B This is the sum of the forces on all the electrons, so the force F acting on each electron is given by

If there is a magnetic field of flux density B at 90° to the current, the conductor will experience a force of magnitude I L B This is the sum of the forces on all the electrons, so the force F acting on each electron is given by I L B I B F = = n A L n A

Substituting for I gives

Substituting for I gives n A L e B F = = t n A

Substituting for I gives n A L e B L e B F = = t n A t

but L/t is

but L/t is the (drift) velocity of the electrons

but L/t is the (drift) velocity of the electrons therefore

but L/t is the (drift) velocity of the electrons therefore F = e v B

In general the magnitude of the force acting on a charged particle moving with velocity v, at 90° to a magnetic field of flux density B, is given by F = q v B where q is the charge on the particle

If the particle moves at angle q to the field

If the particle moves at angle q to the field the magnitude of the component of its velocity at 90° to the field is

If the particle moves at angle q to the field the magnitude of the component of its velocity at 90° to the field is v cos a

If the particle moves at angle q to the field the magnitude of the component of its velocity at 90° to the field is v cos a = v sin q Therefore, in general F =

If the particle moves at angle q to the field the magnitude of the component of its velocity at 90° to the field is v cos a = v sin q Therefore, in general F = q v B sin q