1 Chapter 29--Examples. 2 Problem a) Derive the equation relating the total charge Q that flows...
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Transcript of 1 Chapter 29--Examples. 2 Problem a) Derive the equation relating the total charge Q that flows...
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Chapter 29--Examples
2
Problem
a) Derive the equation relating the total charge Q that flows through a search coil (Conceptual Example 29.3 in Section 29.2) to the magnetic field B. The search coil has N turns, each with area A and the flux through the coil is decreased from its initial value to zero in a time t. The resistance of the coil is R and the total charge is Q=I t where I is the average current induced by the change in flux
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From Example 29.3
A search coil is a practical way to measure magnetic field strength. It uses a small, closely wound coil with N turns. The coil, of area A, is initially held so that its area vector A is aligned with a magnetic field with magnitude B. The coil is quickly pulled out of the field or rotated.
Initially the flux through the field is =NBA. When it leaves the field or rotated, goes to zero. As decreases, there is a momentary induced current which is measured. The amount of current is proportional to the field strength.
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Solution
EMF=-/t–
Where =NBA and =0
EMF=NBA/tV=iR where V=EMF
EMF=NBA/t=iR i=NBA/Rt
Q=it=NBA/R
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Part B
In a credit card reader, the magnetic strip on the back of the card is “swiped” past a coil within the reader. Explain using the ideas of the search coil how the reader can decode information stored in the pattern of magnetization in the strip.
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Solution
The card reader contains a search coil.The search coil produces high EMF and
low EMF as the card is swiped.A high EMF is treated as a binary 1 and
a low EMF is treated as a binary 0Ascii information (character codes
between 1 and 64) can be stored there in a few bits (6-bits or 26).
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Problem
A circular loop of flexible iron wire has an initial circumference of 165 cm but its circumference is decreasing at a rate of 12 cm/s due to a tangential pull on the wire. The loop is in a constant, uniform magnetic field oriented perpendicular to the plane of the loop and with a magnitude of 0.5 T
a) Find the EMF induced in the loop at the instant when 9 s have passed.
b) Find the direction of the current in the loop as viewed looking in the direction of the magnetic field.
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EMF=-/t=-B*A/t
=BA d/dt=BdA/dt c=2r so A=r2
r=c/2 so A=c2/4 dA/dt=d/dt(c2/4c/4)dc/dt d/dt= Bc/2)dc/dt
Where B=0.5 dc/dt=0.12 m/s At 9s, c=1.65-.12*(9s)=0.57 m
d/dt=5.44 x 10-3 V Since is decreasing, the EMF is positive. Since
EMF positive, point thumb along A and look at fingers. They curl counterclockwise.
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Problem
Suppose the loop in the figure below is a) Rotated about the y-axisb) Rotated about the x-axisc) Rotated about an edge parallel to the z-axis.What is the maximum induced EMF in each case if A=600 cm2, w=35
rad/s, and B=.45T?
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Case a—Rotating about y-axis
VBAEMF
tBAtBAdt
dtbut
BAdt
dAB
dt
d
dt
dEMF
945.035*06.0*45.0
sincos
cos
max
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Case b—rotating about the x-axis
The normal to the surface is in the same direction as B during this rotation. Thus BA=constant
d/dt(constant)=0 so EMF=0
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Case c—Rotating about z-axis
VBAEMF
tBAtBAdt
dtbut
BAdt
dAB
dt
d
dt
dEMF
945.035*06.0*45.0
sincos
cos
max
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Problem
The figure below shows two parallel loops of wire having a common axis. The smaller loop (radius r) is above the larger loop (radius R) by a distance x>>R. Consequently, the magnetic field due to current i in the larger loop is nearly constant throughout the smaller loop. Suppose that x is increasing at a constant rate, v.
1) Determine the magnetic flux though area of the smaller loop as a function of x.
2) In the smaller loop find1) The induced EMF2) The direction of the induced current.
x
Radius=r
Radius=R
i
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Magnetic Field of a Circular Loop
3
20
23
22
20
22 x
iR
Rx
iRB
By the RH Rule, the field is upward in the small ring
23
20
23
20
2
2
rx
iRAB
rAandx
iRB
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EMF in smaller loop
42
20
43
32
202
3
20
23
20
3
2
31
1
22
2
xvr
iREMF
vdt
dxbut
dt
dx
xxdt
d
xdt
dr
iRr
x
iR
dt
d
dt
dEMF
rx
iRAB
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Direction of current
Assume that normal to smaller loop is positive upwards
B, then, is in positive directionBut is decreasing or has a negative d
d /dtA negative * negative=positive so EMF is
+RH Thumb in up direction, fingers curl
counter clockwise!