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 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.

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

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 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.

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.

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

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

Two parallel wires carrying currents in the same direction experience an attractive force between them.

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

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

Two parallel wires carrying currents in the same direction experience an attractive force between them.

The magnetic field inside a solenoid carrying current is given by B = μ₀nI, where n is the number of turns per unit length.

In Biot-Savart Law, 'dL' represents an infinitesimal element of length along the current-carrying conductor.

'dl' represents the infinitesimal length of the wire segment that contributes to the magnetic field at a point.

The symbol μ₀ represents the magnetic permeability of free space, which is a constant used in the Biot-Savart Law.

A 'current element' refers to a small segment of wire carrying current, which contributes to the overall magnetic field.

The magnetic field at the center of a circular loop of radius R carrying current I is given by B = μ₀I/(2R) and for a complete loop, it simplifies to B = μ₀I/(2πR).

The Biot-Savart Law describes the magnetic field generated by a steady current flowing through a conductor.

The magnetic field produced by a current-carrying loop at its center is perpendicular to the plane of the loop, following the right-hand rule.

The direction of the magnetic field produced by a current-carrying wire is perpendicular to both the wire and the direction of the current.

According to the right-hand rule, if you point your thumb in the direction of the current, your fingers curl in the direction of the magnetic field.

According to the Biot-Savart Law, the magnetic field strength is inversely proportional to the distance, so doubling the distance halves the magnetic field strength.

Increasing the current in a wire increases the magnetic field around it, as per the Biot-Savart Law.

According to the Biot-Savart Law, the magnetic field strength decreases with increasing distance from the current-carrying wire.