\( 0.5 \, \text{N/m} \)
\( 1 \, \text{N/m} \)
Given:
The formula for the force per unit length on a current-carrying wire in a magnetic field is: \[ \frac{F}{L} = B I \sin \theta \] where: - \( \frac{F}{L} \) is the force per unit length, - \( B \) is the magnetic field strength, - \( I \) is the current, - \( \theta \) is the angle between the magnetic field and the current.
\[ \frac{F}{L} = (0.5 \, \text{T}) \times (2 \, \text{A}) \times \sin(30^\circ) \] Since \( \sin(30^\circ) = 0.5 \), we get: \[ \frac{F}{L} = 0.5 \times 2 \times 0.5 = 0.5 \, \text{N/m} \]
The force per unit length on the wire is \( \boxed{0.5 \, \text{N/m}} \).
Two long parallel wires separated by distance ‘d’ carry currents I1 and I2 in the same direction. They exert a force F on each other. Now the current in one of the wire is increased to three times and its direction is made opposite. The distance between the wires is doubled. The magnitude of force between them is
A photon of energy ‘E’ ejects photoelectrons from a metal surface whose work function is W0. If this electron enters into uniform magnetic field of induction ‘B’ in a direction perpendicular to field and describes a circular path of radius‘r’, then radius is given by