Find Induced Voltage in Rotating Conductor in Radial Field

In summary, the problem is asking for the induced voltage in a conductor rotating in a radius of 25 cm at 1200 rev/min, with a magnetic field given by B = 0.5 a_{r}. While voltage is typically induced in a closed circuit, it can also be induced in any material over a length dL using the equation dV = (B x dL) * v. This is because the magnetic field causes a force that makes the electrons "want" to move along the wire. The work done per charge can be calculated using the equation V = vBL, where v is the velocity of the element of length dL. However, in this case where v changes along the rod, the work
  • #1
erece
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Homework Statement


A conductor 1 cm in length is parallel to z axis and rotates in a radius of 25 cm at 1200 rev/min , find induced voltage if radial field is given by B = 0.5 a[itex]_{r}[/itex]

Homework Equations





The Attempt at a Solution


i am confused. If there is no closed path then how the voltage can be induced
 
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  • #2
Voltage (actually emf) is induced in any material of any kind - even a vacuum! - over a length dL:

dV = (B x dL) * v
where B is magnetic field and v is the velocity of the element of length dL. Vectors in bold.

The direction of dL is in the direction of conventional current under the assumption of a closed circuit. But there need not be a closed circuit.
 
  • #3
hi erece! :smile:
erece said:
If there is no closed path then how the voltage can be induced

the magnetic field causes a force, so that the electrons to "want" to move along the wire

whether they can is irrelevant … there is a gravitational potential difference between the table and the floor even if the things on the table cannot fall to the floor! :biggrin:

voltage = potential energy difference per charge = work done per charge (V = W/q)

work done = force "dot" displacement

for example, if a rod of length L moves at speed v perpendicularly to a uniform magnetic field B, then the force on a charge q inside the rod is qvB along the rod,

so the work done moving it a distance L along the rod is ∫ qvB dx = qvBL,

and the work done per charge is vBL,

ie V = vBL​

ok, that's for linear motion, where v is constant (along the rod) …

in your case, v changes along the rod, so the work done integral (∫ qvB dx) will be more complicated :smile:
 

FAQ: Find Induced Voltage in Rotating Conductor in Radial Field

What is induced voltage in a rotating conductor in a radial field?

Induced voltage in a rotating conductor in a radial field is the voltage generated in a conductor when it moves through a magnetic field. This motion creates a change in the magnetic flux, which in turn induces an electric field and voltage in the conductor.

How is induced voltage calculated in a rotating conductor in a radial field?

The induced voltage in a rotating conductor in a radial field can be calculated using the equation E = BLv, where E is the induced voltage, B is the magnetic field strength, L is the length of the conductor, and v is the velocity of the conductor.

What factors affect the induced voltage in a rotating conductor in a radial field?

The induced voltage in a rotating conductor in a radial field is affected by the strength of the magnetic field, the length of the conductor, and the velocity at which the conductor moves through the field. It is also affected by the angle between the magnetic field and the conductor, as well as the number of turns in the conductor.

What is the direction of induced voltage in a rotating conductor in a radial field?

The direction of the induced voltage in a rotating conductor in a radial field is determined by the right-hand rule. If the fingers of the right hand point in the direction of the magnetic field, and the palm faces the direction of motion of the conductor, then the thumb will point in the direction of the induced voltage.

What are some practical applications of induced voltage in a rotating conductor in a radial field?

Induced voltage in a rotating conductor in a radial field is used in various applications, such as generators, motors, and transformers. It is also used in devices like microphones and speakers, where the motion of the conductor produces an electrical signal that can be amplified and converted into sound waves.

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