When a magnetic field is applied perpendicular to a loop of wire, the magnetic flux through the loop is maximized, resulting in maximum induced EMF according to Faraday's law.

Using the right-hand rule, point your thumb in the direction of the velocity (to the right) and your fingers in the direction of the magnetic field (into the page). Your palm will face out of the page, indicating the direction of the force.

Magnetic flux (Φ) = B * A = B * πr². Here, A = π(0.1)² = 0.01π m². Thus, Φ = 0.1 * 0.01π = 0.01π Wb ≈ 0.0314 Wb.

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

Using the formula F = BIL, where B is the magnetic field, I is the current, and L is the length of the wire (1 m), F = 0.1 T * 5 A * 1 m = 0.5 N.

Using Ampere's Law, B = μ₀I/2πr, where μ₀ = 4π × 10^-7 Tm/A, we find B = (4π × 10^-7)(5)/(2π(0.1)) = 0.1 T.

The magnetic field at the center of a semicircular arc of radius R carrying current I is given by B = μ₀I/(4R).

The magnetic field at the center of a semicircular wire carrying current I is given by B = μ₀I/(4R) for the semicircle, which is half of the full circular loop.

The magnetic field at the center of a semicircular wire carrying current I is given by B = μ₀I/(4R).

If the angle is 90 degrees, the sine of the angle is zero, resulting in zero contribution to the magnetic field from that current element.

Magnetic flux (Φ) is given by Φ = B * A. If the area (A) is doubled, the magnetic flux also doubles.

Magnetic flux Φ is given by Φ = B * A. If the area A is doubled while B remains constant, the magnetic flux also doubles.

Induced EMF is proportional to the area of the loop. If the area is doubled, the induced EMF also doubles.

The magnetic field at the center of a loop is directly proportional to the current.

The magnetic field at the center of a circular loop is directly proportional to the current; thus, if the current is doubled, the magnetic field also doubles.

The magnetic field at the center of the loop is directly proportional to the current.

According to the Biot-Savart Law, increasing the current in a circular loop increases the magnetic field at the center of the loop.

Reversing the current in a circular loop reverses the direction of the magnetic field at the center.

The magnetic field strength around a coil is directly proportional to the current, so if the current is doubled, the magnetic field strength will also double.

Reversing the current in a coil reverses the direction of the magnetic field produced.

The magnetic field inside a solenoid is directly proportional to the current.

The magnetic field is directly proportional to the current, so it doubles.

According to Biot-Savart Law, the magnetic field is directly proportional to the current. Therefore, if the current is doubled, the magnetic field also doubles.

According to Ampere's Law, the magnetic field is directly proportional to the current, so doubling the current will double the magnetic field.

According to the Biot-Savart Law, the magnetic field is directly proportional to the current, so if the current is doubled, the magnetic field also doubles.

Reversing the current in a wire reverses the direction of the magnetic field around it.

Reversing the current in a wire also reverses the direction of the magnetic field around it.

The time period (T) is the reciprocal of frequency (f). T = 1/f = 1/60 Hz = 0.0167 s.

Capacitive reactance X_C = 1/(ωC) decreases as frequency increases.

Inductive reactance X_L = 2πfL = 2π(50)(2) = 628 Ω.