A proton traveling along the \(x\) -axis at a speed of \(1.0 \cdot 10^{6} \mathrm{~m} / \mathrm{s}\) enters the gap between the plates of a \(2.0-\mathrm{cm}-\) wide parallel plate capacitor. The surface charge distributions on the plates are given by \(\sigma=\pm 1.0 \cdot 10^{-6} \mathrm{C} / \mathrm{m}^{2}\). How far has the proton been deflected sideways \((\Delta y)\) when it reaches the far edge of the capacitor? Assume that the electric field is uniform inside the capacitor and zero outside.

Short Answer

Expert verified
Answer: The sideways deflection of the proton when it reaches the far edge of the capacitor is 4.32 x 10^-4 m.

Step by step solution

01

Calculate the electric field inside the capacitor

Using the relation between electric field (E) and surface charge density (σ), we can find the electric field inside the capacitor: \(E = \frac{\sigma}{\epsilon_0}\) where \(ε_0\) is the vacuum permittivity (\(8.85 \cdot 10^{-12} \mathrm{C}^2 / \mathrm{N}\mathrm{m}^2\)). \(\sigma = 10^{-6} \mathrm{C}/\mathrm{m}^2\) \(E = \frac{10^{-6} \mathrm{C}/\mathrm{m}^2}{8.85 \cdot 10^{-12} \mathrm{C}^2 / \mathrm{N}\mathrm{m}^2} = 1.13 \cdot 10^5 \mathrm{N}/\mathrm{C}\)
02

Determine the force acting on the proton

The force acting on the proton due to the electric field can be calculated using: \(F = qE\) where \(q\) is the charge of the proton (\(1.6 \cdot 10^{-19} \mathrm{C}\)). \(F = (1.6 \cdot 10^{-19} \mathrm{C})(1.13 \cdot 10^5 \mathrm{N}/\mathrm{C}) = 1.81 \cdot 10^{-14} \mathrm{N}\)
03

Calculate the acceleration of the proton in the y-direction

Using Newton's second law, we can find the acceleration of the proton in the y-direction: \(F = ma\) \(a = \frac{F}{m}\) where \(m\) is the mass of the proton (\(1.67 \cdot 10^{-27} \mathrm{kg}\)). \(a = \frac{1.81 \cdot 10^{-14} \mathrm{N}}{1.67 \cdot 10^{-27} \mathrm{kg}} = 1.08 \cdot 10^{13} \mathrm{m}/\mathrm{s}^2\)
04

Calculate the time taken for the proton to travel across the width of the capacitor

Using the initial speed \(v_x = 1.0 \cdot 10^6 \mathrm{m}/\mathrm{s}\) and the width of the capacitor \(d = 2.0 \mathrm{cm} = 0.02 \mathrm{m}\), we can find the time taken for the proton to travel across the width: \(t = \frac{d}{v_x} = \frac{0.02 \mathrm{m}}{1.0 \cdot 10^6 \mathrm{m}/\mathrm{s}} = 2.0 \cdot 10^{-8} \mathrm{s}\)
05

Calculate the sideways deflection (Δy) of the proton

Using the time \(t\) and the acceleration \(a\) found in the previous steps, we can calculate the sideways deflection (Δy) of the proton: Δy = \(\frac{1}{2}at^2\) Δy = \(\frac{1}{2}(1.08 \cdot 10^{13} \mathrm{m}/\mathrm{s}^2)(2.0 \cdot 10^{-8} \mathrm{s})^2 = 4.32 \cdot 10^{-4} \mathrm{m}\) Therefore, the sideways deflection of the proton when it reaches the far edge of the capacitor is \(4.32 \cdot 10^{-4} \mathrm{m}\).

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