To determine the value of \( x \), we must first find the electric field magnitude in the region where a proton travels undeflected due to balanced crossed electric and magnetic fields.
The proton moves at a constant speed of \( 2 \times 10^5 \, \text{m/s} \) when the electric field \( \mathbf{E} \) and magnetic field \( \mathbf{B} \) are mutually perpendicular and of such strengths that their forces on the proton negate each other:
The electric force is \( F_E = qE \), where \( q \) is the proton's charge.
The magnetic force on the proton moving at speed \( v \) in field \( \mathbf{B} \) is \( F_B = qvB \), where \( B \) is the magnetic field strength.
For zero net force, \( F_E = F_B \).
Therefore, \( qE = qvB \), which simplifies to:
\( E = vB \)
Next, consider the scenario when the electric field is absent:
The proton follows a circular path, indicating the magnetic force acts as the centripetal force for a circular trajectory with radius \( r = 0.02 \, \text{m} \).
The centripetal force is \( F_c = \frac{mv^2}{r} \).
Equating the magnetic and centripetal forces yields \( qvB = \frac{mv^2}{r} \).
This equation simplifies to:
\( B = \frac{mv}{qr} \)
Substitute the known values: \( m = 1.6 \times 10^{-27} \, \text{kg} \), \( v = 2 \times 10^5 \, \text{m/s} \), \( q = 1.6 \times 10^{-19} \, \text{C} \), and \( r = 0.02 \, \text{m} \):
\( B = \frac{1.6 \times 10^{-27} \times 2 \times 10^5}{1.6 \times 10^{-19} \times 0.02} \approx 0.01 \, \text{T} \)
Now, substitute \( B = 0.01 \, \text{T} \) and \( v = 2 \times 10^5 \, \text{m/s} \) into the equation for \( E \):
\( E = 2 \times 10^5 \times 0.01 = 2000 \, \text{N/C} \)
The electric field magnitude is \( 2000 \, \text{N/C} \), equivalent to \( 2 \times 10^3 \, \text{N/C} \). Given the conversion \( x \times 10^4 \, \text{N/C} = E \):
\( x \times 10^4 = 2000 \Rightarrow x = 0.2 \)
Thus, the value of \( x \) is 0.2.
The magnetic field at the centre of a current carrying circular loop of radius \(R\) is \(16\,\mu\text{T}\). The magnetic field at a distance \(x=\sqrt{3}R\) on its axis from the centre is ____ \(\mu\text{T}\).
