2022 A/L Physics Past Paper · Question 50 (English Medium)

The x part of the magnetic field of a long wire along a semicircle round it

A long straight wire placed at the origin OO carries a constant current directed out of the paper along the ZZ-axis. Figure shows a semicircle of radius RR drawn on the XX-YY plane centering the wire. Which one of the following graphs best represents the variation of the xx-component of the magnetic flux density (Bx)(B_x) along the semicircular path with xx?

  1. (1) Graph (1)
  2. (2) Graph (2)
  3. (3) Graph (3)
  4. (4) Graph (4)
  5. (5) Graph (5)
Answer and explanation

Answer: (2) Graph (2)

What the question asks

What we know:

A very long straight wire passes through the origin OO, along the ZZ-axis. The current comes out of the paper, towards us.

The semicircle has radius RR and its centre is the wire. It is the upper half, on the side where yy is positive.

There are no numbers, so we keep the letters.

We want: the graph of BxB_x against xx along the semicircle.

What each letter means:

II (A\text{A}): the current in the wire.

RR (m\text{m}): the radius of the semicircle, the distance of every point of it from the wire.

B0B_0 (T\text{T}): the size of the magnetic flux density at distance RR from the wire.

BxB_x (T\text{T}): the xx-part of the magnetic flux density.

xx, yy (m\text{m}): the position of a point on the semicircle, measured from the wire.

Relevant theory

What is happening:

The wire makes a magnetic field that goes round it in circles.

Every point of the semicircle is the same distance RR from the wire. So the size of the field is the same, B0B_0, at every point of the semicircle.

The field points along the circle. With the current out of the paper, it goes round anticlockwise.

At the top of the semicircle, going anticlockwise means pointing to the left. At the right end it points up. At the left end it points down.

We want only the xx-part of the field. So we look at how far the field points to the right or to the left.

Then the iron powder will be found to set around the wire along concentric circular paths indicating the presence of a magnetic field and also its structure.

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.

B=μ0I2πrB = \dfrac{\mu_0 I}{2\pi r}

The first quote says that the field goes round the wire in circles.

The second quote gives the direction. A right handed corkscrew moving out of the paper turns anticlockwise when we look at it from the front. So the field goes anticlockwise.

The third quote gives the size, μ0I2πr\dfrac{\mu_0 I}{2\pi r}. It depends on the distance rr from the wire and on nothing else about the point. On the semicircle r=Rr = R everywhere.

For example, a roundabout in a playground that turns anticlockwise. A child at the top of it moves to the left. A child at its right edge moves straight up. Each child moves at the same speed, but the direction keeps turning.

Required equations

B0=μ0I2πRB_0 = \dfrac{\mu_0 I}{2\pi R}

Bx=−B0 yRB_x = -B_0\,\dfrac{y}{R}

Bx≤0B_x \leq 0

Bx=−B0 at x=0,Bx=0 at x=±RB_x = -B_0 \text{ at } x = 0, \quad B_x = 0 \text{ at } x = \pm R

Reasoning and calculation

B0B_0 is in T\text{T}. The fraction yR\dfrac{y}{R} has no unit, so BxB_x is in T\text{T}.

The minus sign comes from the direction. Anticlockwise at a point above the xx axis points a little to the left, towards −x-x.

00

Bx=−B0×0RB_x = -B_0 \times \dfrac{0}{R}

−0.5B0-0.5 B_0

Bx=−B0×0.5B_x = -B_0 \times 0.5

−B0-B_0

Bx=−B0×1B_x = -B_0 \times 1

So BxB_x goes from 00 at the end, to below zero, to its lowest value −B0-B_0 at the top, and back to 00 at the other end. It never goes above zero.

That is a hollow below the axis, touching zero at x=−Rx = -R and at x=Rx = R. It is graph (2).

Check the five graphs.

Graph (1) stays constant, but the direction of the field keeps turning.

Graph (3) is above zero. That is for a current into the paper.

Graphs (4) and (5) change sign at x=0x = 0. BxB_x stays below zero on the whole semicircle.

Graph (2) is below zero, lowest at x=0x = 0 and zero at both ends. It matches.

Checks

−b0∗y/r-b0 * y / r

Does it make sense?

The size of the whole field is the same all along the semicircle. The xx-part is the whole field only at the top, where the field points left. At the two ends the field points straight up or straight down, and the xx-part is zero. That fits graph (2).

The graph must be the same on the left and on the right of x=0x = 0, because the field has the same size and the same tilt at two points the same distance from the yy axis. Graph (2) is.

Conclusion

graph (2)\text{graph }(2)

BxB_x is below zero, lowest at x=0x = 0 and zero at x=±Rx = \pm R. The graph is (2).

The answer is (2).

Find the direction first. Current out of the paper makes the field go anticlockwise round the wire.

The size is the same at the same distance. For the xx-part, ask where the field points to the left, to the right, or straight up and down.

Exam tip

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