A triangular coil of N equal turns lies in the x-y plane with
one corner located at the origin. The total resistance of the coil is R
and the coil is bathed in a spatially uniform, time dependent, magnetic
field at an angle f with the z-axis.
N=14 turns
a=30.0 cm
b=40.0 cm
R=2.40 W
B(t)=0.600 T-(0.250 T/s)t
f = 24.0o
(a) [10 pts] Calculate the total magnetic flux passing the coil
(equation only).
FB
=
NBAcosf
=
(14 turns)[0.600 T-(0.250 T/s)t](0.500)(0.300 m)(0.400 m) cos24.0o
=
0.460 Wb-(0.192 Wb/s)t
(b) [10 pts] Calculate the current induced in each turn of the coil.
Eind
=
-
dFB
dt
=
+0.192 Wb/s
=
+0.192 V
iind
=
Eind
R
=
0.192 V
2.40 W
=
7.79×10-2 V
�
77.9 mV
(c) [5 pts] In the diagram, draw in the direction of Bind. Also,
looking in along the z-axis towards the origin, draw in the direction of the
current flow.
ANS: CCW
A constant, external mechanical force F=Fy [^(j)]
is applied to a slide wire segment [`ab] causing it to move with
constant speed, v. The slide wire contacts a U-shaped wire having resistance
R to form a complete electrical circuit. The system is bathed in a uniform
magnetic field, B=+B [^(k)]. The constants are
R=0.100 W
Lab=15.0 cm
B=0.750 T
v=2.40 m/s
(a) [5 pts] Which point, a or b, is at the higher electrical
potential?
ANS: Point b is at the higher potential. Use the right-hand-rule.
(b) [5 pts] Calculate the induced emf in the slide wire.
Eind
=
BvLab
=
(0.750 T)(2.40 m/s)(0.150 m)
=
0.270 V
(c) [5 pts] Calculate the magnitude of the induced electric field
in the slide wire.
E
=
E
Lab
=
0.270 V
0.150 m
=
1.80 V/m
(d) [5 pts] Calculate the magnitude of the mechanical force applied to
the slide wire.
Fmech
=
ILabB
=
ELabB
R
=
(0.270 V)(0.150 m)(0.750 T)
0.100 W
=
0.304 N
(e) [5 pts] Calculate the power dissipated in the slide wire.
P
=
Fmechv
=
(0.304 N)(2.40 m/s)
=
0.729 W
The diagram shows a single turn circular wire symmetrically placed
inside a single turn square coil (both lie in the same plane). The mutual
inductance of the combination is M. A time-dependent current cource
powers the square wire. A switch is also located in the square wire.
M=8.60×10-3 H
i(t)=(4.80 A)e-0.200t
(a) [8 pts] At t=0, switch S is closed. At what rate is the
current changing in the square wire at t=0.120 s?
di1
dt
=
(4.80 V)(-0.200/s)e-(0.200/s)(0.120 s)
=
-0.937 A/s
(b) [7 pts] Calculate the induced emf in the circular wire at
t=0.120 s.
E2
=
-M21
di1
dt
=
-(8.60×10-3 H)(-0.937 A/s)
=
8.06×10-3 V
�
8.06 mV
(c) [4 pts] In the figure, draw in the direction of the induced
current in the circular wire.
ANS: CCW
(d) [6 pts] If the current source and switch are now removed from the
square wire and inserted into the circular wire and the process in part (a)
is repeated, what are the induced voltage and the corresponding current
direction in the square wire at t=0.120 s?
ANS: E2=8.06 mV CCW
The direction of the induced electric field is CCW everwhere.
The figure shows a simple circuit containing a battery, switch, resistor
and, a REAL inductor.
Eb=95.0 V
R=30.0 W
RL=50.0 W
L=8.00 mH
(a) [5 pts] Calculate the value of the inductive time constant,
tL.
tL
=
L
Rtot
=
8.00×10-3 H
30.0 W+ 50.0 W
=
1.00×10-4 s
(b) [5 pts] When the switch is just closed at t=0, what is the
magnitude of the induced emf in the inductor?
ANS: 95.0 V
(c) [5 pts] At t=5.00×10-5 s, calculate the net current
in the circuit.
i(t)
=
If(1-e-t/tL)
=
� �
95.0 V
80.0 W
� �
(1-e-(5.00× 10-5 s)/(1.00×10-4 s))
=
0.467 A
(d) [5 pts] At t=5.00×10-5 s, calculate the induced emf
in the inductor.
E
=
iR+EL
EL
=
95.0 V-(0.467 A)(80.0 W)
=
57.6 V
(e) [5 pts] At t=5.00×10-5 s, at what rate is the net
current changing?
EL
=
-L
di
dt
di
dt
=
-
E
L
=
-
57.6 V
8.00×10-3 H
=
-7.20×103 A/s
FORMULAS
E=-N dFB/dt
FB=
� �
S
B·
^
n
dA
V=IR
UL=Li2/2
i=if(1-e-t/tL)
N2F2=M21i1
E2=-M21 di1/dt
tL=L/R
E=BLv
E=EL
P=F·v
P=E2/R
F=IL×B
E=-Ldi/dt
File translated from
TEX
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TTH,
version 3.85. On 27 Apr 2016, 10:31.