2019 A/L Physics Past Paper · Question 17 (English Medium)

Electric field at A due to a distribution of point charges

The magnitude and the direction of the electric field at point AA due to the point charge distribution shown in the figure are

  1. (1) 2q4πε0a2\dfrac{2q}{4\pi\varepsilon_0 a^2} →
  2. (2) q4πε0a2\dfrac{q}{4\pi\varepsilon_0 a^2} ↑
  3. (3) 2q4πε0a2\dfrac{2q}{4\pi\varepsilon_0 a^2} ←
  4. (4) 6q4πε0a2\dfrac{6q}{4\pi\varepsilon_0 a^2} ↑
  5. (5) 6q4πε0a2\dfrac{6q}{4\pi\varepsilon_0 a^2} ↓
Answer and explanation

Answer: (1) 2q4πε0a2\dfrac{2q}{4\pi\varepsilon_0 a^2} →

What the question asks

We want:

The size and the direction of the electric field at AA.

Eight point charges are around AA on a square grid.

Relevant theory

The field of a point charge QQ at a distance rr is:

E=Q4πε0r2E = \dfrac{Q}{4\pi\varepsilon_0 r^2}

It points away from a positive charge and towards a negative charge.

With many charges, the fields add as vectors.

Also, field intensity is a vector quantity and its direction is represented by the direction of the force acting as this positive charge.

Applying it to this question

The sources, seen from AA:

+3q+3q above, at aa.

+3q+3q below, at aa.

+q+q on the left, at aa.

−q-q on the right, at aa.

Four +q+q at the corners, each at 2 a\sqrt{2}\,a.

Signs:

+x+x to the right and +y+y up.

A positive charge pushes the field away from it. A negative charge pulls it towards it.

Reasoning and calculation

Upper and lower +3q+3q

Ey=0E_y = 0

Each gives 3q4πε0a2\dfrac{3q}{4\pi\varepsilon_0 a^2}.

The upper one points down. The lower one points up.

They are equal and opposite. They cancel.

The four corner +q+q

E⃗corner=0\vec E_{corner} = 0

Each gives q4πε0(2a)2=q8πε0a2\dfrac{q}{4\pi\varepsilon_0 (\sqrt{2}a)^2} = \dfrac{q}{8\pi\varepsilon_0 a^2}.

Opposite corners are at equal distances on opposite sides of AA.

They cancel in pairs.

The left +q+q

E=q4πε0a2 →E = \frac{q}{4\pi\varepsilon_0 a^2}\ \rightarrow

Its field points away from +q+q, to the right.

Its size is q4πε0a2\dfrac{q}{4\pi\varepsilon_0 a^2}.

The right −q-q

Its field points towards −q-q, also to the right.

Add them as vectors.

The vertical parts cancel.

The corners give zero.

The two horizontal parts point the same way, to the right.

E=q4πε0a2+q4πε0a2=2q4πε0a2E = \frac{q}{4\pi\varepsilon_0 a^2} + \frac{q}{4\pi\varepsilon_0 a^2} = \frac{2q}{4\pi\varepsilon_0 a^2}

Reading the options

The size is 2q4πε0a2\dfrac{2q}{4\pi\varepsilon_0 a^2} and the direction is to the right.

That is option (1).

Option (3) has the same size but the opposite direction.

Why the other options fail

This option has a vertical field. There is none.

The direction is reversed.

This option does not cancel the +3q+3q charges.

Checks

A check by symmetry.

If −q-q were +q+q, the picture would be fully symmetric. The field at AA would be zero.

Our sum would then give q−q=0q - q = 0. So only the −q-q breaks the symmetry.

Conclusion

E=2q4πε0a2 →E = \frac{2q}{4\pi\varepsilon_0 a^2}\ \rightarrow

The symmetric pairs cancel.

The left +q+q and the right −q-q both give a field to the right.

So the field is 2q4πε0a2\dfrac{2q}{4\pi\varepsilon_0 a^2} to the right.

The answer is option (1).

When the field of many charges is asked, first find the pairs that cancel.

Then work out only what is left.

Exam tip

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