2021 A/L Physics Past Paper · Question 33 (English Medium)

Magnetic field at a corner of a square with three wires

Three long straight conducting wires AA, BB and CC are kept at the three vertices of a square as shown in the figure. They are parallel to each other and carry equal currents of II directed out of the plane of the paper. The direction of the resultant magnetic flux density at point DD is given by,

  1. (1) aa
  2. (2) bb
  3. (3) cc
  4. (4) dd
  5. (5) ee
Answer and explanation

Answer: (1) aa

What the question asks

We want: the direction of the total magnetic field at the corner DD.

Three long wires stand at three corners of a square. Each wire carries the same current II. The current comes out of the paper, towards you.

The plan: first find what each wire does at DD on its own. Then add the three.

Relevant theory

When a right handed corkscrew is passed in the direction of an electric current passing through a conductor, the sense of rotation of the screw represents the direction of the magnetic field formed around the conductor.

According to the structure of the composite field, the two fields have added with each other to form a stronger field on the left side of the conductor while on the right side of the conductor the two fields oppose each other resulting a weaker field.

Applying it to this question

Think of a roundabout in a park. Children run round and round it.

Each wire is like a roundabout. Its magnetic field goes round and round the wire, in circles.

At any spot, the field points along the circle. It never points straight at the wire or straight away from it.

A long wire makes this field at a distance rr:

B=μ0I2πrB = \dfrac{\mu_0 I}{2\pi r}

In words: a spot that is farther from the wire gets a weaker field.

Which way does each field point at DD? Use the corkscrew rule. The current comes out of the paper, so the field goes round each wire anticlockwise.

Now look at the three wires one by one.

Wire AA

B1B_1, down and to the right

Wire AA is a distance xx from DD, up and to the right. Its field is BA=μ0I2πxB_A = \dfrac{\mu_0 I}{2\pi x}. Call this B1B_1.

Going anticlockwise round AA, the field at DD points down and to the right.

Wire CC

B1B_1, down and to the left

Wire CC is also a distance xx from DD, down and to the right. Its field is BC=B1B_C = B_1.

Going anticlockwise round CC, the field at DD points down and to the left.

Wire BB

0.71 B10.71\,B_1, straight down

Wire BB is across the square, a distance 2 x\sqrt{2}\,x from DD, straight to the right. It is farther away, so it is weaker: BB=B12=0.71 B1B_B = \dfrac{B_1}{\sqrt{2}} = 0.71\,B_1.

Going anticlockwise round BB, the field at DD points straight down.

Reasoning and calculation

Now add the three. Split each push into a sideways part and a down part.

Sideways: AA pushes right and CC pushes left, both by 0.71 B10.71\,B_1. It is like two children pulling a rope with the same strength in opposite ways. Nothing moves. They cancel.

Down: wire AA gives 0.71 B10.71\,B_1, wire CC gives 0.71 B10.71\,B_1 and wire BB gives 0.71 B10.71\,B_1. All three point down, so they add.

00

0.71 B1−0.71 B10.71\,B_1 - 0.71\,B_1

2.12 B12.12\,B_1

0.71 B1+0.71 B1+0.71 B10.71\,B_1 + 0.71\,B_1 + 0.71\,B_1

The sideways part is zero. The down part is 2.12 B12.12\,B_1.

So the total field at DD points straight down. Straight down is arrow aa.

Reading the options

The arrows are: aa down, bb down and right, cc right, dd up and right, ee up.

Straight down is aa. This is option (1).

Why the other options fail

Arrow bb is the push of wire AA only. Wire CC cancels its sideways part.

The field of a wire goes round the wire. It never points along the line to the wire.

Arrow dd points straight at wire AA. A wire's field goes round it.

Arrow ee is the opposite way. The field goes anticlockwise round a wire with the current coming out of the paper.

Checks

Does it make sense?

Look at the picture. Wires AA and CC are the same distance from DD, one above and one below.

So their sideways pushes must be equal and opposite. Only a push straight down (or straight up) can be left.

3∗a/b3 * a / b

Conclusion

BD=3×0.71 B1=2.12 B1 (down)B_D = 3 \times 0.71\,B_1 = 2.12\,B_1 \text{ (down)}

The sideways parts of AA and CC cancel. The down parts of AA, BB and CC add up to 2.12 B12.12\,B_1.

The total field at DD points straight down, along arrow aa. The answer is (1).

Each wire's field goes round the wire. Use the corkscrew rule for the way.

Split every push into sideways and down parts, and add the parts one direction at a time.

Exam tip

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