1. Initial Kinetic Energy and Path Radius:
The kinetic energy \( K \) of a charged particle with mass \( m \) and velocity \( v \) is defined as:
\[ K = \frac{1}{2} m v^2 \]
When subjected to a uniform magnetic field, the particle follows a circular trajectory with radius \( r \), calculated as:
\[ r = \frac{mv}{qB} \]
Where:
2. Impact of Halving Kinetic Energy:
Upon passing through the lead sheet, the particle's kinetic energy is reduced by half. The resulting kinetic energy \( K' \) is:
\[ K' = \frac{1}{2} K = \frac{1}{2} \times \frac{1}{2} m v^2 = \frac{1}{4} m v^2 \]
Given that kinetic energy is proportional to the square of velocity, the particle's new velocity \( v' \) will be:
\[ v' = \frac{v}{\sqrt{2}} \]
The radius of the particle's new path, \( r' \), is determined by:
\[ r' = \frac{m v'}{q B} \]
Substituting the expression for \( v' \) into this equation yields:
\[ r' = \frac{m \frac{v}{\sqrt{2}}}{q B} = \frac{r}{\sqrt{2}} \]
Radius Conclusion:
3. Time Period of Revolution:
The time period \( T \) for a particle's revolution in a magnetic field is given by:
\[ T = \frac{2 \pi m}{q B v} \]
As the particle's velocity decreases to \( v' = \frac{v}{\sqrt{2}} \), the new time period \( T' \) becomes:
\[ T' = \frac{2 \pi m}{q B v'} \]
Substituting \( v' \) into this equation results in:
\[ T' = \frac{2 \pi m}{q B \frac{v}{\sqrt{2}}} = \sqrt{2} \times \frac{2 \pi m}{q B v} = \sqrt{2} \times T \]
Time Period Conclusion:
Overall Summary:
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.