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Chapter 30. Serway & Beichner. Force between two current carrying wires. Electric current The A mpere - PowerPoint PPT Presentation
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Chapter 30
Serway & Beichner
Force between two current carrying wires
Electric current The Ampere
The ampere is that constant current which, if maintained in two straight parallel conductors of infinite length, of negligible circular cross-section, and placed 1 m apart in vacuum, would produce a force between them equal to 2 × 10-7 Newton per meter of length.
Fig 30-8, p.932
Fig 30-9c, p.933
Fig 30-1, p.927
Fig 30-3, p.929
120
0
coscos4
sin4
2
1
aI
daIB
See Ex. 30.1
Fig 30-7, p.931
See Ex. 30.3
2/322
20
axis2 Rz
IRB
R
I2
0 @ z = 0
3
20
2zIR
z >> R
Ch. 30 10
Fig 30-17, p.938
Fig 30-12, p.935
rIB
2
0
rRIB 2
0
2
for r > R
for r < R
Application of Ampère’s Law
Fig 30-19, p.939
nI
IlNB
0
0
Field inside Solenoid
start
9/13/04
Fig P30-20, p.940
Magnetic Flux
B = B•dA = BAcos
Ampère’s Law One More Time
Ampere’s law states that the line integral of B . ds around any closed loop equals oI where I is the total steady current passing through any surface bounded by the closed loop.
Surface
oIldB
Now introduce a capacitor to interrupt the the circuit. If our power supply is strong enough to keep I constant, the gray surface will give B = 0!
What’s wrong?
Assume that I is constant.
Apply Ampère’s Law to either the,white or gray surfaces, both of which are bounded by the red loop.This leads to:
rIB
2
0
If the power supply can keepthe current constant, the cap.will be charged: +Q/-Q onleft/right plate. This establishesan E-field between the two plates.
E = E•dA = Q/o
Electric flux will change in time corresponding to an effective current called the Displacement Current
dtdQ
dtd
o
Consider to different surfaces
Slide 39 Fig 30-26, p.943
Fig 30-27, p.945
Orbital Motion of the Electron in an Atom
Fig 30-28, p.946
Magnetic Moments due to Spin of electron, neutron and proton
Table 30-1, p.946
Electron Proton neutron
-928 1.41 -0.966
Magnetic Moments 10-26 J/T
Polarization
Generated Field points in the opposite direction
Table 30-2, p.948
Paramagnetism
0M
Generated field adds to applied field
Atomic currents
Diamagnetism0M Generated field opposes applied field
Magnetic Domains
The Earth as a big magnet