We have a current-carrying coil in a magnetic field B. Torque is τ, θ is the angle between the normal to the plane of the coil and B, and φ is the flux linked with the coil. We need to analyze the relationship between τ, φ, and θ.
The torque on a current-carrying coil in a magnetic field is given by:
\(\tau = B I A N \sin\theta\)
Where:
The magnetic flux through the coil is given by:
\(\phi = B A N \cos\theta\)
Where:
When \(\theta = 90^\circ\):
When \(\theta = 0^\circ\):
Given the choices and having accurately computed everything, the correct choice is if the answer's correct value read: τ is zero and φ is maximum for θ : 0°
Solution: - The torque \( \tau \) on a current-carrying coil in a magnetic field is given by: \[ \tau = N I A B \sin \theta \] where \( N \) is the number of turns, \( I \) is the current, \( A \) is the area of the coil, \( B \) is the magnetic field strength, and \( \theta \) is the angle between the normal to the plane of the coil and the magnetic field. - When \( \theta = 0^\circ \), the normal to the coil is aligned with the magnetic field, so the torque \( \tau = 0 \). - The flux \( \varphi \) linked with the coil is given by: \[ \varphi = B A \cos \theta \] For \( \theta = 0^\circ \), \( \cos 0^\circ = 1 \), so \( \varphi \) is maximum. Thus, \( \tau \) is zero and \( \varphi \) is maximum when \( \theta = 0^\circ \).
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of