How Slow Must an Electron Travel to Reach the Opposite Plate in a Capacitor?

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In summary, the slowest speed an electron can have to reach the negative plate in a parallel-plate capacitor charged to ±1.0 nC with plates spaced 1.0 cm apart is -1.13 x 10^-10 m/s. This is determined by using the equations C=EoA/d and \DeltaV=Q/C, and the electron will experience a potential difference of 1.13 x 10^-10 V as it travels from the positive plate to the negative plate.
  • #1
nckaytee
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A parallel-plate capacitor is formed of two 10 cm × 10 cm plates spaced 1.0 cm apart. The plates are charged to ±1.0 nC. An electron is shot through a very small hole in the positive plate.
a. What is the slowest speed the electron can have if it is to reach the negative plate (Hint: set final speed
at negative plate equal to zero)?

I used C=EoA/d (8.85 x 10^-12)(100 x 10^-2)/(1 x 10^-2) = 8.85

Then I used [tex]\Delta[/tex]V=Q/C 0 - Vi = (1 x 10^-9)/8.85

So, Vi = -1.13 x 10^-10

Can anyone verify this for me?
 
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  • #2


I can verify that your calculations are correct. The slowest speed an electron can have in order to reach the negative plate is -1.13 x 10^-10 m/s. This is because the electron will experience a potential difference of 1.13 x 10^-10 V as it travels from the positive plate to the negative plate, and this potential difference is equal to the initial kinetic energy of the electron. Therefore, the initial velocity of the electron must be equal to this potential difference divided by its mass, which is -1.13 x 10^-10 m/s.
 
  • #3


I can verify your calculations. Your approach and equations are correct. The initial velocity of the electron, Vi, should indeed be -1.13 x 10^-10 m/s in order to reach the negative plate with a final speed of zero. This means that the electron must be shot with a speed of -1.13 x 10^-10 m/s or faster in order to reach the negative plate. Any slower and it will not have enough kinetic energy to overcome the electric field between the plates and reach the negative plate.
 

Related to How Slow Must an Electron Travel to Reach the Opposite Plate in a Capacitor?

1. What is a parallel-plate capacitor?

A parallel-plate capacitor is an electrical component that stores energy in an electric field between two parallel conductive plates. It consists of two plates separated by a dielectric material.

2. How does a parallel-plate capacitor work?

When a voltage is applied to the parallel-plate capacitor, an electric field is created between the plates. This field causes a buildup of opposite charges on each plate, creating a potential difference between them. The capacitor can then store energy in this electric field.

3. What factors affect the capacitance of a parallel-plate capacitor?

The capacitance of a parallel-plate capacitor is affected by the distance between the plates, the surface area of the plates, and the type of dielectric material used. The closer the plates are, the larger the surface area, and the higher the permittivity of the dielectric material, the higher the capacitance will be.

4. How is the capacitance of a parallel-plate capacitor calculated?

The capacitance of a parallel-plate capacitor can be calculated using the formula C = ε0A/d, where C is the capacitance, ε0 is the permittivity of free space, A is the surface area of the plates, and d is the distance between the plates.

5. What are some common uses for parallel-plate capacitors?

Parallel-plate capacitors are commonly used in electronic circuits to store energy, filter noise, and stabilize voltage. They are also used in power factor correction, energy storage systems, and high-voltage applications.

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