Charged Particle in an Electric Field
HSC Physics Syllabus
- investigate and quantitatively derive and analyse the interaction between charged particles and uniform electric fields, including: (ACSPH083)
-
model qualitatively and quantitatively the trajectories of charged particles in electric fields and compare them with the trajectories of projectiles in a gravitational field
Charges in Uniform Electric Fields
This video analyses the interaction between charged particles and uniform electric fields, deriving the relevant syllabus equations. The video also qualitatively and quantitatively compares the trajectory of charged particles in electric fields to that of projectiles in gravitational fields.
Electric Field Strength
When two parallel charged plates are connected to a potential difference, they produce a uniform electric field with strength:
`E=V/d`
where,
- E is the electric field strength (Vm-1 or NC-1)
- V is the potential difference or voltage (V)
- d is the perpendicular distance between the two parallel plates (m).
The direction of the electric field always goes from the positively charged plate to the negatively charged plate, as shown below.

`E=10/5=2` Vm-1 downwards
A charged particle experiences a force when in an electric field. Positively charged particles are attracted to the negative plate, and negatively charged particles are attracted to the positive plate. The magnitude of this force is given by the equation:
`F_E=qE`
where,
- F is the force (N)
- q is the charge of the particle (C)
- E is the electric field strength (Vm-1 or NC-1)
The electric field strength can therefore be also expressed in the form:
`E=F/q`
Now, since,
then,
`F/q=V/d`
By Newton’s Second law (F = ma), any charged particle in an electric field experiences acceleration. Hence, their change in displacement increases with time, making their trajectory curved (parabolic) rather than linear.
Qualitative and Quantitative Comparison: Electric and Gravitational Fields
Feature |
Motion in Electric Field |
Motion in Gravitational Field |
Shape of trajectory |
Parabolic (for uniform electric fields) |
Parabolic |
Is constant force experienced by projectile? |
Yes, in uniform electric fields. |
Yes, in uniform gravitational fields. |
Can be analysed by vector resolution into horizontal and vertical components? |
Yes |
Yes |
Horizontal component of motion |
Constant |
Constant |
What undergoes motion? |
Charged particles |
Any type of matter |
Magnitude of acceleration |
Typically much larger due to projectiles being of very small mass |
Typically much smaller, due to projectiles being of larger mass. |
Magnitude of forces |
Depends on different parameters than gravitational force.
F = qE (force per unit charge)
|
Depends on different parameters than electric force
F = mg (force per unit mass)
|
Direction of force |
Depends on nature of charge of projectile:
|
Always attractive towards centre of mass of source of gravitational attraction. |
Why Gravity is Not Considered for Motion of Electric Charges
Charged particles experience negligible amounts of gravitational force. For example, an electron on the surface of Earth has gravitational force of magnitude:
Next section: Work Done in Electric Fields