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Magnetic Force Physics 102 Professor Lee Carkner Lecture 18

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Magnetic Force. Physics 102 Professor Lee Carkner Lecture 18. PAL #17 Magnetic Field. Direction electron is fired into magnetic field that points north if it is deflected up Force equation: F = qvB sin q q = sin -1 [(1.7X10 -14 )/((1.6X10 -19 )(3X10 5 )(0.5))] q = - PowerPoint PPT Presentation

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Page 1: Magnetic Force

Magnetic Force

Physics 102Professor Lee

CarknerLecture 18

Page 2: Magnetic Force

PAL #17 Magnetic Field

Direction electron is fired into magnetic field that points north if it is deflected up

Force equation: F = qvB sin = sin-1 [(1.7X10-14)/((1.6X10-19)(3X105)

(0.5))] = v vector points 45 west of north, which is

pointed northwest, so electron was fired from southeast

Page 3: Magnetic Force

Electron in B Field

vB

North

West

South

East

From right hand rule:

B is north and force is up so v is from west

(reversed to east for electron)

Page 4: Magnetic Force

A beam of electrons is pointing right at you. What direction would a magnetic field have to have to produce the maximum deflection in the right direction?

A) RightB) LeftC) UpD) DownE) Right at you

Page 5: Magnetic Force

A beam of electrons is pointing right at you. What direction would a magnetic field have to have to produce the maximum deflection in the up direction?

A) RightB) LeftC) UpD) DownE) Right at you

Page 6: Magnetic Force

A beam of electrons is pointing right at you. What direction would a magnetic field have to have to produce no deflection?

A) RightB) LeftC) UpD) DownE) Right at you

Page 7: Magnetic Force

Electric and Magnetic Force How do the electric and magnetic forces differ?

Dependences Magnetic force depends on v and , as well as B and q

Vector

Force vector does change for a magnetic field, since as the particle is deflected the v vector changes

Page 8: Magnetic Force

Particle Motion A particle moving freely in a magnetic field will

have one of three paths, depending on Straight line

Circle

Helix

This assumes a uniform field that the particle

does not escape from

Page 9: Magnetic Force

Circular Motion

Page 10: Magnetic Force

Circular Motion If the particle moves at right angles to the field the

force vector will cause the path to bend

The particle will move in a circle How big is the circle?

Magnetic force is F = Centripetal force is F =

We can combine to getr = mv/qB

Radius of orbit of charged particle in a uniform magnetic field

Page 11: Magnetic Force

Circle Properties

Circle radius is inversely proportional to q and B

r is directly proportional to v and m

Can use this idea to make mass spectrometer

Send mixed atoms through the B field they will

come out separated by mass

Page 12: Magnetic Force

Today’s PAL

How long would it take an electron to complete one circular orbit around a 1 G magnetic field?

Page 13: Magnetic Force

Helical Motion If the initial velocity is not completely perpendicular

to the field, instead of a circle you get a spiral or helix Charged particles will spiral around magnetic field

lines

For example, if the lines begin and end at a pole

Examples: Gyrosynchrotron radio emission from planets and stars

Page 14: Magnetic Force

Helical Motion

Page 15: Magnetic Force

Solar Wind Particles in Earth’s Magnetic Field

Page 16: Magnetic Force

Magnetic Field and Current Since a current is moving charge, a magnet

will produce a force on a wire with a current flowing through it

So qv = IL, thus:F = BIL sin

We can use the right hand rule to get the

direction of the force Use the direction of the current instead of v

Page 17: Magnetic Force

Force on a Wire

Page 18: Magnetic Force

Force on a Loop of Wire

Consider a loop of wire placed so that it is lined up with a magnetic field Two sides will have forces at right angles

to the loop, but in opposite directions The loop will experience a torque

Page 19: Magnetic Force

Loop of Current

Page 20: Magnetic Force

Torque on Loop For a loop of width w and height h, force is F = BIL sin

for each long side Since = 90 and L = h,

The torque is the force times the moment arm

(distance to the center), which is w/2 Total torque = but hw is the area of the loop, A

If the field is at angle to the loop then

Page 21: Magnetic Force

Torque on Loop

Page 22: Magnetic Force

General Loops If there are multiple loops (N), the torque is the sum of

each = IBAN sin

A loop placed along a magnetic field will try to align such that the field goes straight through it

Can harness the spin to do work Called a motor

Page 23: Magnetic Force

Next Time

Read 20.7-20.8 Homework: Ch 20, P 4, 17, 38, 49 Exam #2 Friday