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Question: A beam of light travelling along x-axis is described by the electric field $E_y = (600 \frac{V}{m}) ...

A beam of light travelling along x-axis is described by the electric field Ey=(600Vm)sinω(txc)E_y = (600 \frac{V}{m}) \sin \omega (t-\frac{x}{c}).

The maximum magnitude of magnetic force on a charge q=2eq = 2e, moving along y-axis with the speed of 3×1023 \times 10^2 m/s is (e=1.6×1019e = 1.6 \times 10^{-19} C)

Answer

1.92 × 10^{-22} N

Explanation

Solution

The problem asks for the maximum magnitude of the magnetic force on a given charge moving in the presence of an electromagnetic wave.

  1. Identify the maximum electric field strength (E0E_0): The electric field is given by Ey=(600Vm)sinω(txc)E_y = (600 \frac{V}{m}) \sin \omega (t-\frac{x}{c}). From this equation, the maximum amplitude of the electric field is E0=600VmE_0 = 600 \frac{V}{m}.

  2. Calculate the maximum magnetic field strength (B0B_0): For an electromagnetic wave, the magnitudes of the electric and magnetic fields are related by the speed of light cc: E0=B0cE_0 = B_0 c Given c=3×108msc = 3 \times 10^8 \frac{m}{s} (speed of light in vacuum). B0=E0c=600Vm3×108ms=2×106 TB_0 = \frac{E_0}{c} = \frac{600 \frac{V}{m}}{3 \times 10^8 \frac{m}{s}} = 2 \times 10^{-6} \text{ T}.

  3. Determine the direction of the magnetic field (B\vec{B}): The light beam travels along the x-axis (direction of propagation). The electric field E\vec{E} is along the y-axis. In an electromagnetic wave, the direction of propagation (k\vec{k}), the electric field (E\vec{E}), and the magnetic field (B\vec{B}) are mutually perpendicular, and their directions are related by k=E×B\vec{k} = \vec{E} \times \vec{B}. Since the propagation is along +x (i^\hat{i}) and E\vec{E} is along +y (j^\hat{j}), then B\vec{B} must be along +z (k^\hat{k}), because i^=j^×k^\hat{i} = \hat{j} \times \hat{k}. So, the magnetic field B\vec{B} oscillates along the z-axis.

  4. Calculate the maximum magnetic force (FB,maxF_{B,max}): The charge q=2e=2×1.6×1019 C=3.2×1019 Cq = 2e = 2 \times 1.6 \times 10^{-19} \text{ C} = 3.2 \times 10^{-19} \text{ C}. The charge moves along the y-axis with a speed v=3×102msv = 3 \times 10^2 \frac{m}{s}. So, the velocity vector v\vec{v} is along the y-axis. The magnetic force on a charge qq moving with velocity v\vec{v} in a magnetic field B\vec{B} is given by FB=q(v×B)\vec{F}_B = q(\vec{v} \times \vec{B}). The magnitude of this force is FB=qvBsinθF_B = q v B \sin \theta, where θ\theta is the angle between v\vec{v} and B\vec{B}. Here, v\vec{v} is along the y-axis and B\vec{B} is along the z-axis. Thus, the angle between them is θ=90\theta = 90^\circ, which means sinθ=1\sin \theta = 1. The maximum magnetic force occurs when the magnetic field is at its maximum magnitude B0B_0. FB,max=qvB0sin90F_{B,max} = q v B_0 \sin 90^\circ FB,max=(3.2×1019 C)×(3×102ms)×(2×106 T)×1F_{B,max} = (3.2 \times 10^{-19} \text{ C}) \times (3 \times 10^2 \frac{m}{s}) \times (2 \times 10^{-6} \text{ T}) \times 1 FB,max=(3.2×3×2)×(1019×102×106) NF_{B,max} = (3.2 \times 3 \times 2) \times (10^{-19} \times 10^2 \times 10^{-6}) \text{ N} FB,max=19.2×10(19+26) NF_{B,max} = 19.2 \times 10^{(-19 + 2 - 6)} \text{ N} FB,max=19.2×1023 NF_{B,max} = 19.2 \times 10^{-23} \text{ N} FB,max=1.92×1022 NF_{B,max} = 1.92 \times 10^{-22} \text{ N}

The final answer is 1.92×1022 N\boxed{1.92 \times 10^{-22} \text{ N}}.

Explanation of the solution:

  1. Obtain maximum electric field E0E_0 from the given equation.
  2. Calculate maximum magnetic field B0B_0 using B0=E0/cB_0 = E_0/c.
  3. Determine the direction of the magnetic field (z-axis) based on the wave propagation (x-axis) and electric field direction (y-axis).
  4. Calculate the maximum magnetic force using FB,max=qvB0sinθF_{B,max} = qvB_0 \sin\theta. Since velocity is along y-axis and magnetic field along z-axis, θ=90\theta = 90^\circ.

Answer: $1.92 \times 10^{-22} \text{ N}