A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).
To solve the problem of determining the magnitude of the electric field \( E \) when a proton is moving undeviated in crossed electric (\( E \)) and magnetic (\( B \)) fields, we need to understand the balance of forces involved. Initially when the proton is undeviated, the electric force must balance the magnetic force:
\( qE = qvB \)
Where:
This simplifies to:
\( E = vB \)
When the electric field is turned off, and the proton moves in a circular path due to only the magnetic force, the centripetal force required for circular motion is provided by the magnetic force:
\( \frac{mv^2}{r} = qvB \)
Where:
Rearranging gives:
\( B = \frac{mv}{qr} \)
Substituting the known values:
\( B = \frac{1.6 \times 10^{-27} \times 2 \times 10^5}{1.6 \times 10^{-19} \times 0.02} \)
\( B = \frac{3.2 \times 10^{-22}}{3.2 \times 10^{-21}} \)
\( B = 0.1 \, \text{T} \)
Substituting \( B \) back into \( E = vB \):
\( E = 2 \times 10^5 \times 0.1 \)
\( E = 2 \times 10^4 \, \text{N/C} \)
Now, the magnitude of the electric field is \( x \times 10^4 \, \text{N/C} \), where \( x = 2 \). According to the problem's expected range, \( x = 2 \) indeed falls within the given range of 1,10, verifying the solution.
Due to presence of an em-wave whose electric component is given by \( E = 100 \sin(\omega t - kx) \, NC^{-1} \), a cylinder of length 200 cm holds certain amount of em-energy inside it. If another cylinder of same length but half diameter than previous one holds same amount of em-energy, the magnitude of the electric field of the corresponding em-wave should be modified as:
The Lagrangian of a particle of mass \( m \) and charge \( q \) moving in a uniform magnetic field of magnitude \( 2B \) that points in the \( z \)-direction, is given by: \[ L = \frac{m}{2} v^2 + qB(x v_y - y v_x) \] where \( v_x, v_y, v_z \) are the components of its velocity \( v \). If \( p_x, p_y, p_z \) denote the conjugate momenta in the \( x, y, z \)-directions and \( H \) is the Hamiltonian, which of the following option(s) is/are correct?
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: