magnetic fields chapter 26 26.2 the force exerted by a magnetic field definition of b
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Magnetic Fields Chapter 26 26.2 The force exerted by a magnetic field Definition of B 26.3 Motion of a charged particle in a magnetic field Applications A circulating charged particle Crossed fields: discovery of the electron The cyclotron and mass spectrometer. - PowerPoint PPT PresentationTRANSCRIPT
Magnetic Fields
Chapter 26
26.2 The force exerted by a magnetic field
Definition of B
26.3 Motion of a charged particle in a magnetic field
Applications
A circulating charged particle
Crossed fields: discovery of the electron
The cyclotron and mass spectrometer
The magnetic field
Magnetic field lines of the earth depicted by
iron filings around a uniformly magnetized
sphere.
Magnetic field lines exit from the north magnetic pole. For the earth this is the geographic south pole.
William Gilbert discovered that the earth
is a natural magnet in 1600.
The definition of B
B is defined in terms of the magnetic force FB exerted on a moving electrically charged particle.
Experimentally it is observed that, when a charge q has velocity v in a magnetic field, there is a force on the charge that is
proportional to q and to v,
greatest when charge moves perpendicular to field, and zero when parallel to the field – in general it is proportional to the sine of the angle between v and B.
perpendicular to both the velocity and the field.
BvqF
Magnetic force and field
The definition of B
BvqF
1N/(A.m)C.m/s
N11T
SI unit of B is the Tesla
Gauss101T 4
The sign of q matters!
Magnetic force and field
CHECKPOINT: An electron moves perpendicular to a magnetic field. What is the direction of B?
A. Left
B. Up
C. Into page
D. Right
E. Down
F. Out of page
Answer: C. For an electron the force is in the direction of – (v x B)
November in Svalbard (Spitsbergen), 80° North
November near Melbourne (Australia), 37° South
Fine structure of the aurora
field-aligned rays, multiple bands, different heights of the lower border, and dynamics!
photos: Jan Curtis
10
Aurora takes many shapes and forms; these are called ‘arcs’ and stretch from one horizon to another
11
The lines within are called rays
12
This is called a ‘corona’ or
crown; it is the view looking
straight up the local magnetic
field line (the magnetic zenith)
13
A particularly bright and
beautiful aurora in the
magnetic zenith
14 – it’s fast!
This view is about half the sky, using a white light camera, at 3 speed
1 frame/second color composite
9°, ~17km
Two cameras superimposed, measuring different wavelengths
(colours)
17
Some questions:
what makes the different colours?
how high is it?
18
Fast incoming particles strike oxygen and nitrogen gases high in the atmosphere, causing them to make light of different colours.
What is the aurora?
19
Auroral Emission Lines
Spectrum of the Sun
Spectrum of the aurora
Energy = h x frequency
Auroral Emission LinesSpectrum of the Sun
Spectrum of the aurora
500 km
100 km
View from the Space Shuttle at 200 km
26.3 Motion of a point charge in a magnetic field
The magnetic force is always perpendicular to the velocity of the particle.
The magnetic force thus changes the direction of the velocity but not its magnitude.
Therefore magnetic fields do no work on particles and do not change their kinetic energy.
The circular path of electrons moving in the magnetic field (into page) produced by two
large coils.
Charged particle moving in a plane perpendicular to a uniform magnetic field
(into page).
A circulating charged particle
False colour photo showing tracks of a 1.6 MeV proton (red) and a 7 MeV alpha particle (yellow) in a cloud chamber.
Radius of curvature is proportional to the momentum, and inversely proportional to the charge.
A circulating charged particle
24
A movie from the TRACE instrument on the SOHO satellite
Our active Sun
25
From the Sun to the Earth
26
27
Sun-to-aurora TV analogy
Helical pathsSuppose that a charged particle enters a uniform magnetic field with a velocity that is not perpendicular to B. There is no force component, and thus no acceleration component parallel to B, so the component of the velocity parallel to B remains constant.
The path of the particle is a helix.
Cloud chamber photo of helical path of an electron in a magnetic field.
Helical paths in a ‘magnetic bottle’ – and in the Earth’s field
A string of auroral “substorms” following a Coronal Mass Ejection (CME) impact on Earth Observed by the University of Iowa’s VIS Imager on the Polar Satellite
Auroral emissions seen from space: the light occurs in two ring shaped regions around each magnetic
pole. Charged particles are guided there by the magnetic field.
31
Aurora on other planets
2 hours of data from IMAGE satellite, measuring Lyman Alpha emissions in ultraviolet from precipitating protons
Svalbard
33
Svalbard
34
Svalbard Radar
where we do some of our research into the aurora
35
First results from new camera ASK (Auroral Structure and Kinetics)
ASK1: 20 seconds of data at 32 fps
18:21:10 – 18:21:30 UT
22 October 2006
3 degree field of view in magnetic zenith
Electric fields acting along the magnetic field
CHECKPOINT: Here are three situations in which a charged particle with velocity v travels through a uniform magnetic field B.
In each situation, what is the direction of the magnetic force FB on the particle? A. LeftB. UpC. Into pageD. RightE. DownF. Out of page
Answers: (a) +z (out)
(b) –x (left, negative particle)
(c) 0
CHECKPOINT: The figure shows the circular paths of two particles that travel at the same speed in a uniform B, here directed into the page. One particle is a proton; the other is an electron.
(a) Which particle follows the smaller circleA. pB. e
(b) Does that particle travel A. clockwise or B. anticlockwise?
Answers: (a) electron (smaller mass)
(b) clockwise
pe
Crossed magnetic and electric fieldsNet force:
The forces balance if the speed of the
particle is related to the field strengths by
qvB = qE
BvqEqF
v = E/B (velocity selector)
Measurement of q/m for electronJ J Thomson 1897
EXERCISE: Find an expression for q/m
Sun-to-aurora TV analogy
41
A small part of the sky overhead