College Physics
College Physics
11th Edition
ISBN: 9781305952300
Author: Raymond A. Serway, Chris Vuille
Publisher: Cengage Learning
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**Example: A proton is released from rest at the positive plate of a capacitor. What is the proton’s speed when it reaches the negative plate? The capacitor is illustrated below with spacing d = 2.1mm. The strength of the electric field is E = 4.5 × 10⁴ N/C.**

![Image of Capacitor](https://example.com/capacitor_image.png)

*Figure 6.26*

First off, note that the acceleration \( a_x \) component is negative because it points to the left so \( a_x = -\frac{qE}{m} \). We choose the velocity squared equation above because we want to solve for the final velocity (and we are not given the time interval):

\[ v_{xf}^2 = v_{xi}^2 + 2a_x (x_f - x_i) = 0 - \frac{2Eq(x_f - x_i)}{m} = -\frac{2Eq x_f}{m} \]

Where we made \( x_i = 0 \) such that \( x_f = 0.0021m \) and that the proton starts at rest so \( v_{xi} = 0 \). We have to take the square root to get the final speed:

\[ v_{xf} = \pm \sqrt{-\frac{2Eq x_f}{m}} \]

And substituting the numbers we get:

\[ v_{xf} = \pm \sqrt{\frac{4.5 \times 10^4 \, N/C \, \times (1.602 \times 10^{-19} \, C) \, \times (-0.0021 \, m)}{-2 \times 1.67 \times 10^{-27} \, kg }} = \pm 1.35 \times 10^5 \, m/s \]

Notice that the sign underneath the radical is positive (as required) and to get the correct velocity component we need to choose the negative sign (moving to the left). The proton is moving extremely fast in this case because typical fields (like in an old TV set) are on this order (around \( 10^5 \, N/C \)).

**Question 7: Homework – Unanswered**

For the example above, how long (in nanoseconds) does it take the proton to travel the distance of 2
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Transcribed Image Text:**Example: A proton is released from rest at the positive plate of a capacitor. What is the proton’s speed when it reaches the negative plate? The capacitor is illustrated below with spacing d = 2.1mm. The strength of the electric field is E = 4.5 × 10⁴ N/C.** ![Image of Capacitor](https://example.com/capacitor_image.png) *Figure 6.26* First off, note that the acceleration \( a_x \) component is negative because it points to the left so \( a_x = -\frac{qE}{m} \). We choose the velocity squared equation above because we want to solve for the final velocity (and we are not given the time interval): \[ v_{xf}^2 = v_{xi}^2 + 2a_x (x_f - x_i) = 0 - \frac{2Eq(x_f - x_i)}{m} = -\frac{2Eq x_f}{m} \] Where we made \( x_i = 0 \) such that \( x_f = 0.0021m \) and that the proton starts at rest so \( v_{xi} = 0 \). We have to take the square root to get the final speed: \[ v_{xf} = \pm \sqrt{-\frac{2Eq x_f}{m}} \] And substituting the numbers we get: \[ v_{xf} = \pm \sqrt{\frac{4.5 \times 10^4 \, N/C \, \times (1.602 \times 10^{-19} \, C) \, \times (-0.0021 \, m)}{-2 \times 1.67 \times 10^{-27} \, kg }} = \pm 1.35 \times 10^5 \, m/s \] Notice that the sign underneath the radical is positive (as required) and to get the correct velocity component we need to choose the negative sign (moving to the left). The proton is moving extremely fast in this case because typical fields (like in an old TV set) are on this order (around \( 10^5 \, N/C \)). **Question 7: Homework – Unanswered** For the example above, how long (in nanoseconds) does it take the proton to travel the distance of 2
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