Rotating Coil in Magnetic Field

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Homework Help Overview

The discussion revolves around calculating the magnetic field (B) using a search coil, based on the charge passing through the coil during its rotation in a magnetic field. The problem involves understanding the relationship between charge, current, resistance, and electromagnetic induction as described by Faraday's law.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between charge, current, and resistance, questioning how to incorporate these into the calculation of magnetic flux change. There are attempts to derive equations linking these concepts, with some participants expressing uncertainty about the role of the coil's area and the number of turns in the calculations.

Discussion Status

The discussion is active, with participants providing insights into the relationships between the variables involved. Some guidance has been offered regarding the need to consider time in Faraday's law, and there is an ongoing exploration of how to correctly apply the equations to arrive at a solution.

Contextual Notes

Participants are navigating the constraints of the problem, including the fixed area of the coil and the need to account for the number of turns in their calculations. There is a recognition of the complexity involved in integrating these concepts correctly.

dukesolice
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Homework Statement


[/B]
Magnetic field values are often determined by using a device known as a search coil. This technique depends on the measurement of the total charge passing through a coil in a time interval during which the magnetic flux linking the windings changes either because of the motion of the coil or because of a change in the value of B. As a specific example, calculate B when a 61-turn coil of resistance 194Ω and cross-sectional area 44.5m^2 produces the following results: A total charge of 4.76E-4C passes through the coil when it is rotated in a uniform field from a position where the plane of the coil is perpendicular to the field to a position where the coil's plane is parallel to the field.

Homework Equations


emf = -change in flux

The Attempt at a Solution



emf = -d/dt (integral of B dot dA)

The change in flux is from when the coil is perpendicular to the field to when the coil is parallel to the field. So 90 degrees. But I don't know how to get the change the in area, and how to use the charge and resistance.
 
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dukesolice said:
But I don't know how to get the change the in area, and how to use the charge and resistance.
The shape of the coil doesn't change as the coil rotates. So, the area of the coil remains constant.

You'll need to bring together several elementary concepts in this problem. How is charge related to current and time? How is current related to resistance and emf?
 
TSny said:
The shape of the coil doesn't change as the coil rotates. So, the area of the coil remains constant.

You'll need to bring together several elementary concepts in this problem. How is charge related to current and time? How is current related to resistance and emf?

Current is charge/time. Emf = current * resistance.
 
dukesolice said:
Current is charge/time. Emf = current * resistance.
OK. These relations along with Faraday's law give you everything you need.

Try combining them to get a relation between the total charge and the change of flux.
 
dukesolice said:

Homework Equations


emf = -change in flux
This is not correct. Faraday's law also involves time.
 
So now I have dQ/dt * R = -d(flux)/dt, so then I took integral of both sides and got NRQ = -BA, where N is number of coils, this gave me the wrong answer
 
dukesolice said:
So now I have dQ/dt * R = -d(flux)/dt,
OK, but should the number of turns, N, appear somewhere here?

so then I took integral of both sides and got NRQ = -BA, where N is number of coils, this gave me the wrong answer
Show the steps in getting to this result. Why does N appear on the left?
 

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