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Ampere is defined as a current at which two very long parallel wires 1 m apart create a force on each other of 2 . 10 -7 N per meter length. From this also follows that 0 /(4) = 10 -7 T . m/A Forces Between Parallel Wires Definition of 1 Ampere:
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Forces Between Parallel Wires

Feb 23, 2016

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Forces Between Parallel Wires. Definition of 1 Ampere:. Ampere is defined as a current at which two very long parallel wires 1 m apart create a force on each other of 2 . 10 -7 N per meter length. From this also follows that  0 /(4) = 10 -7 T . m/A. Forces Between Parallel Wires. - PowerPoint PPT Presentation
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Page 1: Forces Between Parallel Wires

Ampere is defined as a current at which two very long parallel wires 1 m apart create a force on each other of 2.10-7 N per meter length.

From this also follows that 0/(4) = 10-7 T.m/A

Forces Between Parallel Wires

Definition of 1 Ampere:

Page 2: Forces Between Parallel Wires

For long wire:

Magnetic force on lower wire: Magnetic force on upper wire:

What if current runs in opposite directions?

Forces Between Parallel Wires

Electric forces: “likes repel, unlikes attract”Magnetic forces: “likes attract, unlikes repel”

Page 3: Forces Between Parallel Wires

Magnetic force acts only on moving charges

Mobile electrons experience magnetic force

The motion of the wire is an electric side-effect of the magnetic force on the moving electrons.

Why does the Wire Move?

Atomic cores are not moving – no magnetic force!Atomic cores feel an unbalanced force. Wire movesdown!

Page 4: Forces Between Parallel Wires

X

Y

Z

Clicker Question

Page 5: Forces Between Parallel Wires

Metal bar

Fm

polarization

Static equilibrium:

Metal is in static equilibrium: but E 0 inside!

What is V ?

Currents Due to Magnetic Forces

Page 6: Forces Between Parallel Wires

Metal bar

Fm

Static equilibrium:

How much force do weneed to apply to keepthe bar moving at constantspeed?

Does this polarized bar remind you anything we’ve already studied?

Currents Due to Magnetic Forces

Page 7: Forces Between Parallel Wires

Fm

Non-Coulomb forcedrives e against FE

Non-Coulomb work:

What is emf of this ‘battery’?

Non-Coulomb work per unit charge:

Bar may have some resistance rint:

‘motional emf’

Non-Coulomb Work

Page 8: Forces Between Parallel Wires

Is round trip V zero?

EE

Round-trip Potential

Yes! Looks like any other emf.

Page 9: Forces Between Parallel Wires

P=IV=I(emf) Are we getting something for nothing?

Fm

Bar – current I:

FI F

Work:

Power:

Main principle of electric generators:Mechanical power is converted to electric power

Moving Bar and Energy Conservation

x

Page 10: Forces Between Parallel Wires

A current carrying loop has a tendency to twist in magnetic field

Compass needle: collection of atomic current loops

Magnetic Torque on a Magnetic Dipole Moment

Page 11: Forces Between Parallel Wires

Torque () = distance from the axle (lever arm) times perpendicular component of the force.

Works with loops of any shape!

Magnetic Torque: Quantitative Analysis

Page 12: Forces Between Parallel Wires

Calculate amount of work needed to rotate from angle I to f:

Potential energy for a magnetic dipole moment

Magnetic Dipole Moment: Potential Energy

Page 13: Forces Between Parallel Wires

Potential energy for a magnetic dipole moment

U= min-µB

0 maxµB

0

What is the energy difference between the highest and the lowest state?

Picture of the U and µ in magnetic field – important in atomic and nuclear physics.

Magnetic Dipole Moment: Potential Energy

Page 14: Forces Between Parallel Wires

charged tape

Any magnetic field?

Reference Frame

Page 15: Forces Between Parallel Wires

Two protons

+e

+e

r

1

2

v

v

Electric force:

E1

F21,e

Magnetic field:

B1 Magnetic force:

F21,m

Magnetic Forces in Moving Reference Frames

Page 16: Forces Between Parallel Wires

Electric force:

Magnetic force:

+e

+e

r

1

2

v

vE1

F21,e

B1

F21,m

Ratio:

(m/s)2

=c2

it is not accidental!

Magnetic Forces in Moving Reference Frames

Page 17: Forces Between Parallel Wires

+e

+e

r

1

2

v

vE1

F21,e

B1

F21,mFor v<<c the magnetic force is muchsmaller than electric force

How can we detect the magnetic force ona current carrying wire?

Full Lorentz force:

Magnetic Forces in Moving Reference Frames

downward

Page 18: Forces Between Parallel Wires

+e

+e

r

1

2

v

vE1

F21,e

B1

F21,mWho will see protons hitfloor and ceiling first?

20 ns

15 ns

Time must run slower in moving frame.

Einstein 1905: “On the electrodynamics of moving bodies”

Magnetic Forces in Moving Reference Frames

Page 19: Forces Between Parallel Wires

There may be different mechanisms for different observers in different reference frames, but all observers can correctly predict what will happen in their own frames, using the same relativistically correct physical laws.

The Principle of Relativity