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Physics Lesson 14.5.8 - Motion of Charged Particles inside a Uniform Field

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Welcome to our Physics lesson on Motion of Charged Particles inside a Uniform Field, this is the eighth lesson of our suite of physics lessons covering the topic of Electric Potential, you can find links to the other lessons within this tutorial and access additional physics learning resources below this lesson.

Motion of Charged Particles inside a Uniform Field

An electric charge Q experiences an electric force Fe when it is inserted inside an electric field. As a result, it experiences an acceleration a, which based on the Newton's Second Law is

a = Fe/m

where m is the mass of the charged particle.

If the charge is too small, the effect of gravity is not taken into account, so the charge will move linearly, in the direction of electric field as shown in the figure.

Physics Tutorials: This image provides visual information for the physics tutorial Electric Potential

Given that Fe = Q × E, we can write for the acceleration caused by the electric force

a = Q × E/m

Example 7

A proton starts moving from the positive towards the negative plate of a system composed by two parallel metal plates charged oppositely as those shown in the figure above. What is the velocity by which the proton collides with the negative plate if the distance between the plates is 20 cm? Take the mass of proton mp = 1.67 × 10-27 kg and the charge of electron Q = 1.6 × 10-19 C.

Physics Tutorials: This image provides visual information for the physics tutorial Electric Potential

Solution 8

First, we must calculate the electric field E between the plates. We have

E = ∆V/d
= 24 V/0.2 m
= 120 V/m
= 120 N/C

Now, let's calculate the acceleration caused by the electric force on the proton. We have

a = Q × E/m
= 1.6 × 10-19 C × 120 N/C/1.67 × 10-27 kg
= 1.15 × 1010 m/s2

Therefore, using the kinematic formula

v2 - v20 = 2 × a × d

we find after substitutions for the speed v by which the proton hits the negative plate:

v = √2 × a × d
= √2 × 1.15 × 1010 × 0.2
= √0.46 × 1010
= 6.78 × 104 m/s

In some cases, especially when the charged object is quite heavy, the gravitational force cannot be neglected. As a result, there is a combination of two forces, electric and gravitational, which determine the trajectory of the charge moving inside a uniform field. Let's consider an example in this regard.

Example 9

A 2 g metal sphere carrying a charge of 40 μC is inserted inside a uniform electric field as shown in the figure.

Physics Tutorials: This image provides visual information for the physics tutorial Electric Potential

What is the potential difference between the plates if the charge remains stationary in the position shown? Take g = 9.81 N/kg.

Solution 9

Since there is equilibrium, we have

Fg = Fe
m × g = Q × E
m × g = Q × ∆V/d

Thus,

∆V = m × g × d/Q
= 2 × 10-3 kg × 9.81 N/kg × 0.3 m/4 × 10-5 C
= 147.15 V

You have reached the end of Physics lesson 14.5.8 Motion of Charged Particles inside a Uniform Field. There are 8 lessons in this physics tutorial covering Electric Potential, you can access all the lessons from this tutorial below.

More Electric Potential Lessons and Learning Resources

Electrostatics Learning Material
Tutorial IDPhysics Tutorial TitleTutorialVideo
Tutorial
Revision
Notes
Revision
Questions
14.5Electric Potential
Lesson IDPhysics Lesson TitleLessonVideo
Lesson
14.5.1The Meaning of Electric Potential
14.5.2Potential Difference (Voltage)
14.5.3Analogy between Gravitation and Electricity recap
14.5.4Potential Difference between two Conducting Spheres
14.5.5The Relationship between Potential Difference and Electric Field
14.5.6Equipotential Surfaces
14.5.7Potential of a Charged Sphere
14.5.8Motion of Charged Particles inside a Uniform Field

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