Physics · Units 3 & 4

Electric Fields

Understand electric fields the easy way, with plain English intuition, an interactive simulation, point charges and uniform fields, worked examples and an auto marked practice test. VCE Physics Units 3 and 4.

Learn

Bring two charges near each other and they feel a force without ever touching. Each charge fills the space around it with an invisible influence called an electric field, and any other charge dropped into that space gets pushed or pulled. The field is just a map that tells you, at every point, which way a charge would be shoved and how hard. Get the map right and the force falls straight out of it.

A field is a force waiting to happen

Here is the whole idea. An electric field is the region around a charge where another charge feels a force. The field has a strength, written EE, measured in newtons per coulomb (which is the same as volts per metre).

  • The field EE exists whether or not anything is sitting in it. It is a property of the space.
  • Drop a charge qq into the field and it feels a force F=qEF = qE, in the direction of the field for a positive charge.

So the field is the cause and the force is the effect. Find the field first, then multiply by the charge to get the force.

The two field shapes you must know

VCE gives you two field shapes, and almost every question is one of them.

The first is the field around a single point charge. It spreads out in all directions and gets weaker as you move away, following an inverse square law:

E=kQr2,k=8.99×109.E = \frac{kQ}{r^2}, \qquad k = 8.99 \times 10^{9}.

Field lines point away from a positive charge and towards a negative charge. Double your distance and the field drops to a quarter, because of the r2r^2 on the bottom.

The second is the uniform field between two parallel charged plates. Here the field is the same strength and direction everywhere between the plates, and the formula is beautifully simple:

E=Vd.E = \frac{V}{d}.

VV is the voltage across the plates and dd is their separation. This is the setup in the diagram below, and the one the worked examples use.

+ + + + + + +− − − − − − −E+Fd

The red arrow F is the force on the small positive charge, and it points the same way as the field, straight from the positive plate towards the negative plate. The light arrows are the field lines: evenly spaced and all the same length, which is exactly what a uniform field looks like. The separation between the plates is d.

Field gives force, every time

This is the line that ties the whole topic together. Once you know the field at a point, the force on any charge sitting there is one multiplication away.

See it for yourself

Drop positive and negative charges onto the canvas, then use the sensors to read the field strength and direction at any point. Place two opposite charges near each other and watch the field lines bend, or line up a row of charges to build something close to the uniform field between two plates.

Interactive simulation, Charges and Fields Source: PhET Interactive Simulations, University of Colorado Boulder (CC BY 4.0)

How to actually solve one

The method is a short, repeatable recipe.

  1. Decide which field shape you have: a point charge or a uniform field between plates.
  2. For a point charge, find the field with E=kQr2E = \dfrac{kQ}{r^2} using k=8.99×109k = 8.99 \times 10^{9}.
  3. For parallel plates, find the field with E=VdE = \dfrac{V}{d}. Keep the separation in metres.
  4. Once you have EE, the force on a charge sitting in it is F=qEF = qE.

Watch the units. A plate separation given in centimetres or millimetres must be converted to metres first, and charges are almost always tiny powers of ten, so track the exponent carefully.

Lock it in with active recall

Cover the answer and say each one out loud before you flip. Rate yourself honestly — the cards you find hard come back sooner, the ones you know are spaced further out.

Active recall

Answer from memory first, then flip. Rate yourself and each card returns on a spaced schedule (1 → 3 → 7 → 16 days).

What is an electric field, and what are its units?
Write the field formula for a point charge and for parallel plates.
Which way do electric field lines point?
How do you find the force on a charge qq sitting in a field EE?
Double the distance from a single point charge. What happens to EE?
Recall · Gravitational Fields
How does the point-charge field compare with gravitational field strength?
Recall · Charged Particles in Fields
What path does a charge follow when it enters a uniform electric field sideways?

See the recipe in action in the Worked Examples tab, then test yourself in Try It.

Worked examples

Worked Example 1Field between two parallel plates

Two parallel plates are 0.0200.020 m apart with a voltage of 100100 V across them. Find the electric field strength between them.

  1. 1

    Between parallel plates the field is uniform, so the strength is just the voltage divided by the separation.

    E=VdE = \dfrac{V}{d}
  2. 2

    Substitute the voltage and the plate separation.

    E=1000.020E = \dfrac{100}{0.020}
  3. 3

    Work out the division. The units are volts per metre, which is the same as newtons per coulomb.

    E=5000 N/C (V/m)E = 5000 \text{ N/C (V/m)}
Answer
E=Vd=1000.020=5000 N/C (V/m)E = \dfrac{V}{d} = \dfrac{100}{0.020} = 5000 \text{ N/C (V/m)}
Worked Example 2Force on a charge in a field

A charge of 2.0×10−62.0 \times 10^{-6} C sits in a uniform field of 50005000 N/C. Find the electric force on it.

  1. 1

    The force on any charge in a field is the charge multiplied by the field strength.

    F=qEF = qE
  2. 2

    Substitute the charge and the field strength.

    F=(2.0×10−6)(5000)F = (2.0 \times 10^{-6})(5000)
  3. 3

    Multiply the two numbers to get the force in newtons.

    F=0.010 NF = 0.010 \text{ N}
Answer
F=qE=(2.0×10−6)(5000)=0.010 NF = qE = (2.0 \times 10^{-6})(5000) = 0.010 \text{ N}

Practice questions

Practice test

Try it yourself

6 questions, 8 marks

Choose your answers, then submit to see your score and the full worked solutions. Multiple choice is marked for you, just like Exam 2 Section A.

Q1.A small positive test charge is placed in an electric field. The direction of the force on it is:

1mark
Need a hint?
The field direction is defined as the direction of the force on a positive charge.

Q2.Two parallel plates are 0.0100.010 m apart with 5050 V across them. The uniform field strength between them is:

1mark
Need a hint?
Use E=VdE = \dfrac{V}{d} with the numbers given.

Q3.A charge of 3.0×10−63.0 \times 10^{-6} C sits in a uniform field of 20002000 N/C. The electric force on it is:

1mark
Need a hint?
Use F=qEF = qE and keep track of the power of ten.

Q4.If you double the distance from a single point charge, the electric field strength at that point becomes:

1mark
Need a hint?
For a point charge E=kQr2E = \dfrac{kQ}{r^2}, so the field depends on the distance squared.

Q5.Two parallel plates are 0.0400.040 m apart with 200200 V across them. Find the uniform electric field strength between the plates, then find the force on a charge of 5.0×10−65.0 \times 10^{-6} C placed between them. Show your working.

3marks

Work this on paper. The worked solution appears once you submit.

Q6.Two positive point charges, +Q+Q and +9Q+9Q, are placed 2020 cm apart. On the straight line between them, the electric field is:

1mark
Need a hint?
The field is zero where the two fields cancel: kQr2=k(9Q)(0.20−r)2\dfrac{kQ}{r^{2}} = \dfrac{k(9Q)}{(0.20-r)^{2}}.

VCAA 2025 Physics Exam, Section A Q8

Frequently asked questions

What actually is an electric field?
It is the region of space around a charge where another charge would feel a push or a pull. The field strength tells you how big a force a one coulomb charge would feel at that spot, measured in newtons per coulomb.
Why is the field between two parallel plates uniform?
Because the field lines run straight from one plate to the other, evenly spaced and the same strength everywhere in between. That is why one simple formula, E equals V divided by d, works no matter where you are between the plates.
Which way do field lines point?
Field lines point away from positive charges and towards negative charges, always in the direction a small positive test charge would be pushed. They never cross and they are closest together where the field is strongest.