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294' Amperes Law

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29-4. Ampere s Law. Same current (parallel or antiparallel) ... 29-4. Ampere s Law. What is the magnitude of the integral ? (2) cw, i1 up, ccw i1 down, ... – PowerPoint PPT presentation

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Title: 294' Amperes Law


1
29-4. Amperes Law
Sign of the current?
ccw up positive
2
29-4. Amperes Law
Same current (parallel or antiparallel) Rank
the loops according to the magnitude of the
integral
d gt a c gtb
3
29-4. Amperes Law
What is the magnitude of the integral ?
  • ccw -i1 i2

(2) cw, i1 up, ccw i1 down, cw i2 up
-i1 -i1 i2
4
29-4. Amperes Law
5
29-4. Amperes Law
6
29-5. Solenoids
Solenoid 50 cm long, diameter 5 cm Current3
A B-field inside 7 mT What is the length of
the wire?
B n (1.26 x 10-6 ) (3) 7 x 10-3 T
n N/(50 x 10-2 )
L N (2 p) (2.5 x 10-2 )
7
29-5. Solenoids
  • No B-Field outside
  • Uniform Inside

8
29-6. Current-Carrying Coil as a Magnetic Dipole
9
29-6. Current-Carrying Coil as a Magnetic Dipole
Solenoid 200 turns, diameter 5 cm Current3
A (1) What is the magnitude of the magnetic
moment? (2) What is the magnitude of the
B-field at axial distance z 80 cm?
m (200) (3) p (2.5 x 10-2 )2 A/m2
B (1.26 x 10-6 )/(2p) x m /(80 x 10-2 )3 T
10
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11
30-3. Faradays Law
Magnetic Flux
12
30-3. Faradays Law
B(t) given. Rank the regions according to the
magnitude of the emf induced in a conducting
loop.
b gt d e gt a c
13
30-3. Faradays Law
a
  • 3 loops are shown.
  • B 0 everywhere except in the circular region
    where B is uniform, pointing out of the page and
    is increasing at a steady rate.
  • Rank the 3 loops according to the magnitude of
    the induced EMF.

b
c
a b gt c
14
30-4. Lenz s Law
If the magnetic flux increases as time goes, what
is the direction of the induced current?
15
30-4. Lenz s Law
  • 100-turn coil of radius 5cm and 5W.
  • Solenoid of diameter 3cm with 200 turns/cm.
  • The solenoid current drops from 2A to zero in
    Dt2ms.
  • What is the current induced in the coil during
    Dt?

16
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17
30-5. Induction and Energy Transfer
  • Flux change in time current
  • Force on a current by the B-field
  • Power dissipation?

18
30-5. Induction and Energy Transfer
  • Induced current in a solid conducting plate
  • Mechanical energy is transferred to thermal energy

19
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20
30-6. Induced E-Fields
Current
E-field
Potential has no meaning if the E-field is
produced by induction
21
30-6. Induced E-Fields
  • A long solenoid has a circular cross-section of
    radius R.
  • The current through the solenoid is increasing at
    a steady rate di/dt.
  • Compute the E-field as a function of the distance
    r from the axis of the solenoid.

r
22
30-6. Induced E-Fields
23
30-6. Induced E-Fields
  • Two versions of Faradays law
  • A varying magnetic flux produces an EMF
  • A varying magnetic flux produces an E-field

24
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25
30-7. Inductors and Inductance
i
Inductor Generate B-flux by current
Inductance L Generate B-flux by current
26
30-7. Inductors and Inductance
Inductance of a solenoid
27
30-8. Self-Induction
Current appears to oppose the increase
B
i
28
30-8. Self-Induction
  • The current in a 10 H inductor is decreasing at a
    steady rate of 5 A/s.
  • If the current is as shown at some instant in
    time, what is the magnitude and direction of the
    induced EMF?
  • Magnitude (10 H)(5 A/s) 50 V
  • Current is decreasing
  • Induced emf must be in a direction that OPPOSES
    this change.
  • So, induced emf must be in same direction as
    current

29
30-9. RL Circuits
  • Set up a single loop series circuit with a
    battery, a resistor, a solenoid and a switch.
  • Describe what happens when the switch is closed.
  • Key processes to understand
  • What happens JUST AFTER the switch is closed?
  • What happens a LONG TIME after switch has been
    closed?
  • What happens in between?

At t0, a capacitor acts like a wire an inductor
acts like a broken wire. After a long time, a
capacitor acts like a broken wire, and inductor
acts like a wire.
30
30-9. RL Circuits
  • Immediately after the switch is closed, what is
    the potential difference across the inductor?
  • (a) 0 V
  • (b) 9 V
  • (c) 0.9 V
  • Immediately after the switch, current in circuit
    0.
  • So, potential difference across the resistor 0
  • So, the potential difference across the inductor
    E 9 V

31
30-5. RL Circuits
  • Immediately after the switch is closed, what is
    the current i through the 10 W resistor?
  • (a) 0.375 A
  • (b) 0.3 A
  • (c) 0
  • Immediately after switch is closed, current
    through inductor 0.
  • Hence, current trhough battery and through 10 W
    resistor is i (3
    V)/(10W) 0.3 A
  • Long after the switch has been closed, what is
    the current in the 40W resistor?
  • (a) 0.375 A
  • (b) 0.3 A
  • (c) 0.075 A
  • Long after switch is closed, potential across
    inductor 0.
  • Hence, current through 40W resistor (3
    V)/(40W) 0.075 A

32
30-9. RL Circuits
  • How does the current in the circuit change with
    time?

i
i(t)
Small L/R
Large L/R
Time constant of RL circuit L/R
t
33
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34
30-10. Energy Stored in a B-Field
30-11. Energy Density of a B-Field
35
30-10. Energy Stored in a B-Field
  • The switch has been in position a for a long
    time.
  • It is now moved to position b without breaking
    the circuit.
  • What is the total energy dissipated by the
    resistor until the circuit reaches equilibrium?
  • When switch has been in position a for long
    time, current through inductor (9V)/(10W)
    0.9A.
  • Energy stored in inductor (0.5)(10H)(0.9A)2
    4.05 J
  • When inductor discharges through the resistor,
    all this stored energy is dissipated as heat
    4.05 J.
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