- Use the relationship between field strength, potential difference and distance in a
uniform electric field to rewrite E, and then solve for the potential difference
between the ends of the wire segment.
Physics principles and equations
The strength of the force exerted by a magnetic field on a charge moving perpendicular
to it is
We will also use the definition of an electric field.
The equation that relates potential difference to electric field strength and distance in a
uniform electric field is
In this case, the distance d is the wire length L.
Step-by-step derivation
We employ the strategy and equations mentioned above and use algebra to solve for
the potential difference.
As the equation indicates, longer wires, higher velocities, and stronger magnetic fields lead to greater induced potential differences. This
derivation considered the case of motion perpendicular to the magnetic field. If the motion were not perpendicular, we would use trigonometry
to determine the component of the motion that was perpendicular to the field. In general, we would conclude that ǻV = LvB sin ș, just as the
magnetic force equalsqvB sin ș.
Potential difference across wire
segment
For motion perpendicular to field:
ǻV = LvB
ǻV = potential difference across wire
L = length of wire
v = speed
B = magnetic field strength
Step Reason
1. FB = FE forces in equilibrium
2. qvB = Eq substitute expressions for forces
3. vB = E divide by q
4. solve given equation for E
5. substitute equation 4 into equation 3
6. ǻV = LvB solve for ǻV
29.6 - Magnetic flux
Magnetic flux is analogous to electric flux. Specifically, magnetic flux is the product of a
surface area with the component of a magnetic field passing perpendicularly through
the surface, just as electric flux is the measure of how much electric field passes
perpendicularly through a surface. The unit for magnetic flux is the weber (Wb). One
weber is one tesla·m^2 , the units for magnetic field strength times those for area.
With both electric and magnetic flux, the cosine of the angle between the field and the
area vector is used to measure the component of the field passing perpendicularly
through the surface. The area vector is normal to the surface and equal in magnitude to
its area.
In Equation 1, you see the equation for magnetic flux. It states that magnetic flux equals
the dot product of the magnetic field and area vectors, which is calculated as the
product of the magnetic field strength, the surface area, and the cosine of the angle ș.
This angle is shown in the diagram.
You will use the concept of magnetic flux, and changes in magnetic flux, to further your
understanding of how changing magnetic fields induce emfs.
Magnetic flux
Amount of field passing through surface
Depends on:
·Field strength at surface
·Amount of surface area
·Angle between field, area vector
(^542) Copyright 2007 Kinetic Books Co. Chapter 29