Magnetic Force on a Moving Charge:
When a charged particle, such as an electron, moves in a magnetic field, it experiences a force given by:
\[ \vec{F} = q (\vec{v} \times \vec{B}) \]
where \(\vec{v}\) is the velocity of the particle and \(\vec{B}\) is the magnetic field.
The direction of the force is perpendicular to both \(\vec{v}\) and \(\vec{B}\).
Magnetic Field Inside a Solenoid:
Inside a long solenoid carrying current, the magnetic field \(\vec{B}\) is uniform and directed along the axis of the solenoid.
Since the electron is moving along the axis, its velocity \(\vec{v}\) is also parallel to \(\vec{B}\).
No Magnetic Force Due to Parallel \(\vec{v}\) and \(\vec{B}\):
Since \(\vec{v} \parallel \vec{B}\), the cross product \(\vec{v} \times \vec{B} = 0\).
Therefore, the magnetic force \(\vec{F} = 0\), and the electron will not experience any force due to the magnetic field.
Conclusion:
The electron will continue to move with uniform velocity along the axis of the solenoid, as there is no force acting on it to change its state of motion.
List-I EM-Wave | List-II Wavelength Range |
---|---|
(A) Infra-red | (III) 1 mm to 700 nm |
(B) Ultraviolet | (II) 400 nm to 1 nm |
(C) X-rays | (IV) 1 nm to \(10^{-3}\) nm |
(D) Gamma rays | (I) \(<10^{-3}\) nm |
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: