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Chapter 29--Examples. Problem.

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Problem

- 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 Dt. The resistance of the coil is R and the total charge is Q=I Dt where I is the average current induced by the change in flux

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 F=NBA. When it leaves the field or rotated, F goes to zero. As F decreases, there is a momentary induced current which is measured. The amount of current is proportional to the field strength.

Solution

- EMF=-DF/Dt
- DF=F2–F1
- Where F1 =NBA and F2 =0
- DF=-NBA
- EMF=NBA/Dt
- V=iR where V=EMF
- EMF=NBA/Dt=iR
- i=NBA/RDt
- Q=iDt=NBA/R

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.

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 0
- Ascii information (character codes between 1 and 64) can be stored there in a few bits (6-bits or 26).

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

- Find the EMF induced in the loop at the instant when 9 s have passed.
- Find the direction of the current in the loop as viewed looking in the direction of the magnetic field.

EMF=-DF/Dt=-B*DA/Dt

- F=BA
- dF/dt=BdA/dt
- c=2pr so A=pr2
- r=c/2p so A=c2/4p
- dA/dt=d/dt(c2/4p)= (2c/4p)dc/dt
- dF/dt= B(c/2p)dc/dt
- Where B=0.5
- dc/dt=0.12 m/s
- At 9s, c=1.65-.12*(9s)=0.57 m
- dF/dt=5.44 x 10-3 V
- Since F is decreasing, the EMF is positive. Since EMF positive, point thumb along A and look at fingers.
- They curl counterclockwise.

Problem

Suppose the loop in the figure below is

- Rotated about the y-axis
- Rotated about the x-axis
- 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?

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

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.

- Determine the magnetic flux though area of the smaller loop as a function of x.
- In the smaller loop find
- The induced EMF
- The direction of the induced current.

Radius=r

Radius=R

x

i

Magnetic Field of a Circular Loop

By the RH Rule, the field is upward in the small ring

Direction of current

- Assume that normal to smaller loop is positive upwards
- B, then, is in positive direction
- But F is decreasing or has a negative d dF /dt
- A negative * negative=positive so EMF is +
- RH Thumb in up direction, fingers curl counter clockwise!

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