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What is called Faraday's law?

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Faraday's Law of Induction is a fundamental principle in electromagnetism that describes how a changing magnetic field induces an electromotive force (EMF) in a conductor. There are two key parts to Faraday's Law:

1. **Faraday's First Law**: This states that a change in the magnetic field within a closed loop of wire induces an EMF in the wire. The magnitude of the induced EMF is directly proportional to the rate of change of the magnetic flux through the loop.

2. **Faraday's Second Law**: This quantifies the induced EMF by stating that the magnitude of the induced EMF (ε) is equal to the negative rate of change of the magnetic flux (Φ) through the loop:
   \[
   \epsilon = -\frac{d\Phi}{dt}
   \]
   where \( \epsilon \) is the induced EMF, \( \frac{d\Phi}{dt} \) is the rate of change of magnetic flux, and the negative sign represents Lenz's Law, which indicates that the direction of the induced EMF opposes the change in magnetic flux.

**Magnetic Flux (Φ)** is defined as:
   \[
   \Phi = B \cdot A \cdot \cos(\theta)
   \]
   where \( B \) is the magnetic field strength, \( A \) is the area of the loop, and \( \theta \) is the angle between the magnetic field and the normal to the surface of the loop.

Faraday's Law is crucial for the operation of many electrical devices, such as transformers, electric generators, and inductors. It essentially forms the basis for understanding how alternating current (AC) is generated and used in various technologies.
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Faraday's law of electromagnetic induction states that a changing magnetic field within a closed loop induces an electromotive force (EMF) in the loop. Specifically, the law can be summarized as follows:

1. The induced EMF in a circuit is directly proportional to the rate of change of the magnetic flux through the circuit.
2. The direction of the induced EMF and current (if the circuit is closed) is such that it opposes the change in magnetic flux that produced it (Lenz's law).

Mathematically, Faraday's law can be expressed as:

\[
\text{EMF} = -\frac{d\Phi_B}{dt}
\]

where \(\Phi_B\) is the magnetic flux.
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