2018 A/L Physics Past Paper · Question 31 (English Medium)

Viscous oil between three plates — velocity vectors

A thin flat plate ZZ is placed midway between two large horizontal plates XX and YY, and the space is filled with a viscous oil as shown in the figure. Now, consider a situation that the plate ZZ is pulled horizontally to the right with constant speed vv and plate YY is pulled horizontally to the left with constant speed v2\dfrac{v}{2} while keeping XX stationary. The velocity vectors of thin oil layers between plates XX and YY are best represented in,

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

Answer: (5) Figure (5)

What the question asks

We know: XX is at rest.

ZZ moves right at vv. YY moves left at v2\frac{v}{2}.

We want: the figure that shows the velocity vectors of the oil layers.

Relevant theory

The change of velocity according to the gap between two layers is called the velocity gradient.

This property of a liquid is called viscosity and the forces are viscous forces.

The oil layer touching a plate moves with that plate.

In the steady state the tangential force is the same on every layer.

So the velocity gradient is constant.

So the speed changes in a straight line with distance.

Required equations

F=−ηAdvdxF = -\eta A \frac{dv}{dx}

dvdx=constant\frac{dv}{dx} = \text{constant}

Reasoning and calculation

The axes.

Up: the height from YY to XX.

Across: the velocity of the layer. To the right is positive.

The speeds at the plates:

00 at XX.

vv at ZZ, to the right.

v2\frac{v}{2} at YY, to the left.

There are two parts.

The upper layer, between ZZ and XX.

The lower layer, between YY and ZZ.

The behaviour changes at plate ZZ.

In the upper layer the speed grows in a straight line from 00 at XX to vv at ZZ.

In the lower layer it changes in a straight line from vv at ZZ to v2\frac{v}{2} to the left at YY.

Where is the speed zero in the lower layer?

The total change is from vv to −v2-\frac{v}{2}, that is 3v2\frac{3v}{2}.

So the speed is zero two-thirds of the way from ZZ. Below that the arrows point left.

The figure we expect:

No arrow at XX.

Going down, the arrows grow to the right. They are longest at ZZ.

Then they shrink and turn round near YY.

At YY they point left with v2\frac{v}{2}.

Reading the options

Only figure (5) matches this.

The longest arrow points right at ZZ. A small arrow points left at YY.

Why the other options fail

This option says: figure (1). The speed at YY is zero.

But YY moves left at v2\frac{v}{2}.

So it is wrong.

This option says: figure (2). A large speed to the right at YY.

But YY moves to the left.

This option says: figure (3). In the lower layer the speed does not change in a straight line.

But the velocity gradient is constant. So it must change in a straight line from vv at ZZ.

This option says: figure (4). The speed at ZZ points left.

But ZZ moves to the right.

Conclusion

00 at XX.

vv at ZZ, to the right.

v2\frac{v}{2} at YY, to the left.

Straight lines in between.

The answer is option (5).

Explore

Viscous oil fills the space between the plates. XX stays still.

ZZ is pulled right at vv. The oil layers nearer ZZ move faster.

YY is pulled left at v2\frac{v}{2}. Below ZZ the speed changes in a straight line.

The arrows grow from XX to ZZ. Then they shrink and turn left. That is figure (5).

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