A transformer is used to increase or decrease the voltage in an AC circuit based on the turns ratio of its coils.

A transformer operates on the principle of electromagnetic induction, transferring energy between coils through a changing magnetic field.

Ampere's Law states that the line integral of the magnetic field B around a closed path is equal to μ₀ times the total current I enclosed by the path.

Ampere's Law states ∮B·dl = μ₀I_enc, where I_enc is the enclosed current.

Ampere's Law states that the line integral of B around a closed loop is μ₀ times the total current through the loop.

Inside a long straight conductor, the magnetic field is zero because the contributions from all parts of the conductor cancel out.

Faraday's law states that the induced EMF is directly proportional to the rate of change of magnetic flux through the circuit.

Faraday's law states that the induced EMF is directly proportional to the rate of change of magnetic flux through the circuit.

The magnetic field dB is proportional to Idl and sin(θ), where θ is the angle between the current element and the line connecting the current element to the point of interest.

The magnetic field at the center of a circular loop of radius R carrying current I is given by B = μ₀I/(2πR).

According to Ampere's Law, the line integral of the magnetic field around a closed loop equals μ₀ times the total current enclosed by the loop.

The magnetic field at the center of a loop is inversely proportional to the radius. If the radius is halved, the magnetic field quadruples.

For points outside the cylinder, B = μ₀I/2πr.

Using Ampere's Law, B = μ₀I/2πR for points outside the cylindrical conductor.

The magnetic field inside a solenoid is given by B = μ₀nI.

Using Ampere's Law, B = μ₀nI where n is the number of turns per unit length.

The magnetic field inside a toroid is given by B = μ₀NI/2πR.

Using Ampere's Law, B = μ₀I/2R at the center of a circular loop.

The magnetic field at the center of a circular loop is given by B = (μ₀I)/(2R).

Using Ohm's law (I = V/R), the induced current I = 20V / 10Ω = 2 A.

The induced EMF is maximized when the conductor moves perpendicular to the magnetic field lines.

The induced EMF is dependent on the speed of the conductor and the strength of the magnetic field it moves through.

According to the right-hand rule applied to the Biot-Savart Law, the magnetic field at the center of a circular loop of current is directed out of the plane of the loop.

According to Ampere's Law, the magnetic field B at a distance r from a long straight conductor carrying current I is given by B = μ₀I/(2πr).

According to Ampere's Law, the magnetic field B around a long straight conductor is given by B = μ₀I/(2πr).

Using the right-hand rule, the magnetic field at a point directly above the wire is directed counterclockwise around the wire.

Using Ampere's Law, the magnetic field B at a distance r from a long straight wire carrying current I is given by B = μ₀I/(2πr).

The magnetic field B at a distance r from a long straight wire carrying current I is given by B = μ₀I/(2πr).

The magnetic field B at a distance r from a long straight wire carrying current I is given by B = μ₀I/(2πr).

The magnetic field B at a distance r from a long straight wire carrying current I is given by B = (μ₀I)/(2πr).