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Which is an example for dynamically induced emf?

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Dynamically induced electromotive force (emf) refers to the emf generated in a conductor due to the movement of the conductor relative to a magnetic field. This type of emf is described by Faraday's Law of Induction, which states that a change in the magnetic environment of a conductor induces an emf. Here’s a detailed example to illustrate this concept:

### Example: Moving a Conductor in a Magnetic Field

**Scenario:**

Imagine you have a rectangular metal rod placed in a uniform magnetic field. The magnetic field is perpendicular to the length of the rod. If you move the rod perpendicularly through the magnetic field, an emf will be induced in the rod.

**How it Works:**

1. **Magnetic Field Setup:**
   - Suppose you have a magnetic field \( B \) that is uniform and directed into the page (or screen).

2. **Conductor Movement:**
   - If the rectangular rod is moved to the right with a constant velocity \( v \), the motion of the rod through the magnetic field causes a change in the magnetic flux through the rod.

3. **Induction of emf:**
   - According to Faraday’s Law, the emf induced (\( \mathcal{E} \)) in the rod is given by:
     \[
     \mathcal{E} = B \cdot v \cdot L
     \]
     where \( L \) is the length of the rod perpendicular to the direction of motion.

4. **Resulting Voltage:**
   - This induced emf can be measured across the ends of the rod. If you connect a voltmeter across the rod, it will show a voltage corresponding to the induced emf.

**Visualizing the Effect:**

Imagine the rod as a simple bar moving through a magnetic field:

- **Before Moving:** There is no emf because the rod is stationary relative to the magnetic field.
- **During Movement:** As the rod moves through the magnetic field, the free electrons in the rod experience a force (Lorentz force) due to the magnetic field, which causes them to accumulate at one end of the rod, creating an electric field and hence an emf.

**Applications:**

This principle is used in various practical applications, such as:

- **Electric Generators:** In a generator, a coil of wire rotates within a magnetic field, dynamically inducing an emf that generates electrical power.
- **Alternators:** In vehicles, alternators use this principle to convert mechanical energy into electrical energy.
- **Induction Meters:** Devices that measure electrical quantities by detecting changes in the magnetic field due to the motion of conductors.

In summary, moving a conductor through a magnetic field is a classic example of dynamically induced emf, demonstrating how motion and magnetic fields interact to generate electrical energy.
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A classic example of dynamically induced electromotive force (EMF) is the operation of an **alternating current (AC) generator**.

Here's a detailed explanation of how it works:

### AC Generator

1. **Basic Principle**: An AC generator operates on Faraday's Law of Electromagnetic Induction, which states that a change in magnetic flux through a coil induces an EMF in the coil. In an AC generator, the magnetic flux through the coil changes dynamically, thus inducing an EMF.

2. **Components**:
   - **Rotor**: This is the rotating part of the generator, often called the armature.
   - **Stator**: This is the stationary part that contains the magnetic field, usually made of permanent magnets or electromagnets.
   - **Commutator** (in DC generators) or **Slip Rings** (in AC generators): These are used to transfer the generated current from the rotating coil to the external circuit.

3. **Operation**:
   - The rotor (or armature) rotates within the magnetic field produced by the stator.
   - As the rotor spins, the amount of magnetic flux through the coils of wire in the rotor changes continuously.
   - According to Faraday's Law, this change in magnetic flux induces an EMF in the rotor coils.
   - In an AC generator, this induced EMF changes direction periodically as the rotor spins, resulting in alternating current.

4. **Dynamic Aspect**: The key feature here is that the magnetic flux through the rotor coils changes continuously as the rotor spins, leading to a dynamically induced EMF. This dynamic change is what characterizes the EMF as being dynamically induced.

In contrast, **static** induction occurs when a change in the magnetic field near a stationary conductor induces an EMF without movement. The AC generator's dynamic change in flux through the moving coils exemplifies dynamically induced EMF.
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