Increasing the speed of the magnet increases the rate of change of magnetic flux through the coil, which increases the induced current according to Faraday's law.

The magnetic susceptibility of a paramagnetic material decreases with increasing temperature.

For most conductors, resistance increases with temperature due to increased lattice vibrations that impede electron flow.

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

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

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 conductor carrying current I is given by B = (μ₀I)/(2πr).

The force experienced by a charge q moving with velocity v in a magnetic field B is given by the Lorentz force law: F = q(v × B), which can be expressed as F = qvB sin(θ), where θ is the angle between the velocity and the magnetic field.

The magnetic force on a charge moving in a magnetic field is given by F = qvB sin(θ), where θ is the angle between the velocity and the magnetic field.

The force experienced by a current-carrying conductor in a magnetic field is known as the Lorentz force.

The force on a charge moving in a magnetic field is given by F = qvBsinθ, where θ is the angle between v and B.

The magnetic force on a charged particle is given by F = qvBsinθ, where q is the charge, v is the velocity, B is the magnetic field, and θ is the angle between v and B.

The total power in a series RLC circuit is given by P = VI cos(φ), where φ is the phase angle.

The total power in an AC circuit is given by P = VI cos(φ), where φ is the phase angle.

The force on a charged particle moving in a magnetic field is given by F = qvB sin(θ), where θ is the angle between the velocity and the magnetic field.

The magnetic field inside a solenoid is given by B = μ₀(nI), where n is the number of turns per unit length.

The magnetic force on a charged particle is given by F = qvBsin(θ), where q is the charge, v is the velocity, B is the magnetic field strength, and θ is the angle between the velocity and the magnetic field.

The magnetic force on a charge moving in a magnetic field is given by F = qvBsinθ, where θ is the angle between v and B.

The magnetic force on a charged particle is given by F = qvBsinθ, where q is the charge, v is the velocity, B is the magnetic field strength, and θ is the angle between v and B.

The total power in a series RLC circuit is given by P = VI cos(φ), where φ is the phase angle.

The impedance Z = √(R^2 + (ωL)^2) in a series R-L circuit.

The impedance Z in a series R-L circuit is given by Z = √(R^2 + (ωL)^2).

At resonance, the impedance of a series RLC circuit is equal to the resistance R.

The induced EMF (ε) is given by Faraday's law as ε = -A(dB/dt), where A is the area of the loop.

According to Faraday's law of electromagnetic induction, the induced EMF is given by ε = -dΦ/dt.

The induced EMF (ε) is given by Faraday's law of electromagnetic induction: ε = -dΦ/dt. If the change in magnetic field is 5 T/s, then ε = 5 V.

The induced EMF (ε) is given by Faraday's law of electromagnetic induction: ε = -dΦ/dt. If the rate of change of magnetic field is 5 T/s, then ε = 5 V.

According to Faraday's law of electromagnetic induction, the induced EMF is given by ε = -dΦ/dt, where Φ is the magnetic flux.

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

Using Ampere's Law, B = μ₀I/2πr for an infinitely long straight wire.