The source of the force acting on a current-carrying conductor placed in a magnetic field is the magnetic interaction between the moving charges (current) in the conductor and the external magnetic field. The force on a current-carrying conductor in a magnetic field is given by: \[ F = I L B \sin(\theta) \] Where:
\( F \) is the force,
\( I \) is the current,
\( L \) is the length of the conductor in the magnetic field,
\( B \) is the magnetic field strength,
\( \theta \) is the angle between the magnetic field and the conductor.
For two long, straight, parallel conductors carrying steady currents \( I_1 \) and \( I_2 \), the force per unit length between them is given by Ampère's law: \[ F = \frac{\mu_0 I_1 I_2}{2 \pi d} \] Where:
\( \mu_0 \) is the permeability of free space,
\( d \) is the distance between the two conductors.
This is the expression for the force between two parallel conductors carrying steady currents, and it defines Ampère's law.
Bittu and Chintu were partners in a firm sharing profit and losses in the ratio of 4 : 3. Their Balance Sheet as at 31st March, 2024 was as follows:
On 1st April, 2024, Diya was admitted in the firm for \( \frac{1}{7} \)th share in the profits on the following terms:
Prepare Revaluation Account and Partners' Capital Accounts.