2023 A/L Physics Past Paper · Question 37 (English Medium)

Change in length of a composite rod that holds a sphere in a liquid

Two rods of negligible mass each of initial length LL and cross-sectional area AA made of materials of Young's moduli Y1Y_1 and Y2Y_2 are connected in series to make a composite rod. One end of the composite rod is firmly fixed to a rigid ceiling as shown in the figure. A sphere of volume VV made of material of density β\beta is connected to the free end of the rod, and the sphere is fully immersed in a liquid of density ρ\rho (β>ρ\beta > \rho). What will be the change of the length of the composite rod?

  1. (1) V(β−ρ)gLA(1Y1+1Y2)\dfrac{V(\beta - \rho)gL}{A}\left(\dfrac{1}{Y_1} + \dfrac{1}{Y_2}\right)
  2. (2) V(β−ρ)gLA(1Y1−1Y2)\dfrac{V(\beta - \rho)gL}{A}\left(\dfrac{1}{Y_1} - \dfrac{1}{Y_2}\right)
  3. (3) AV(β−ρ)gL(1Y1+1Y2)\dfrac{A}{V(\beta - \rho)gL}\left(\dfrac{1}{Y_1} + \dfrac{1}{Y_2}\right)
  4. (4) AV(β−ρ)gL(Y1−Y2)\dfrac{A}{V(\beta - \rho)gL}\left(Y_1 - Y_2\right)
  5. (5) V(β−ρ)gLA(Y1+Y2)\dfrac{V(\beta - \rho)gL}{A}\left(Y_1 + Y_2\right)
Answer and explanation

Answer: (1) V(β−ρ)gLA(1Y1+1Y2)\dfrac{V(\beta - \rho)gL}{A}\left(\dfrac{1}{Y_1} + \dfrac{1}{Y_2}\right)

What the question asks

We want: the change ee in the length of the composite rod.

What each letter means:

ee (m\text{m}): the total extension of the composite rod.

e1e_1, e2e_2 (m\text{m}): the extensions of the first and the second rod.

LL (m\text{m}) and AA (m2\text{m}^2): the length and the area of each rod.

Y1Y_1, Y2Y_2 (N m−2\text{N m}^{-2}): the Young's moduli of the rods.

VV (m3\text{m}^3): the volume of the sphere.

β\beta, ρ\rho (kg m−3\text{kg m}^{-3}): the density of the sphere and of the liquid.

TT (N\text{N}): the pull in the rods.

gg (m s−2\text{m s}^{-2}): the acceleration of gravity.

Relevant theory

The ratio of tensile stress to tensile strain is called the Young's modulus of the material

of the wire.

When a body is completely or partially immersed in a fluid at rest, it experiences an upthrust equal to the weight of the fluid displaced by the body.

The first quote says what Young's modulus is: the tensile stress divided by the tensile strain. The second quote says that a body in a liquid feels an upthrust equal to the weight of the liquid it pushes aside.

For example, hang a heavy bag from two elastic bands joined end to end. Each band holds the full pull of the bag, and each band stretches.

The bag stretches the pair by the stretch of the first band plus the stretch of the second.

Required equations

W=VβgW = V\beta g

U=VρgU = V\rho g

T=W−U=V(β−ρ)gT = W - U = V(\beta - \rho)g

e1=TLAY1,e2=TLAY2e_1 = \dfrac{T L}{A Y_1}, \quad e_2 = \dfrac{T L}{A Y_2}

e=e1+e2=V(β−ρ)gLA(1Y1+1Y2)e = e_1 + e_2 = \dfrac{V(\beta - \rho)gL}{A}\left(\dfrac{1}{Y_1} + \dfrac{1}{Y_2}\right)

Reasoning and calculation

The pull in the rods:

The sphere hangs at rest. The rod pulls it up with the pull TT, and the liquid pushes it up with the upthrust UU. Its weight WW pulls it down.

So T+U=WT + U = W, which gives T=W−UT = W - U.

The rods have a negligible mass, so each rod carries the same pull TT: the lower rod holds the sphere, and the upper rod holds the lower rod and the sphere.

V(β−ρ)gV(\beta - \rho)g

T=Vβg−Vρg=V(β−ρ)gT = V\beta g - V\rho g = V(\beta - \rho)g

The two extensions add up:

Each rod has the same LL, the same AA and the same pull TT. The moduli are different.

The rod of Y1Y_1 stretches by TLAY1\dfrac{TL}{AY_1}. The rod of Y2Y_2 stretches by TLAY2\dfrac{TL}{AY_2}. The change of the whole length is the sum.

2020

T=0.001×2000×10T = 0.001 \times 2000 \times 10

0.20.2

e1=20×210−6×2×1011e_1 = \dfrac{20 \times 2}{10^{-6} \times 2 \times 10^{11}}

0.40.4

e2=20×210−6×1011e_2 = \dfrac{20 \times 2}{10^{-6} \times 10^{11}}

0.60.6

e=e1+e2e = e_1 + e_2

v∗(b−r)∗g∗l/a∗(1/y1+1/y2)∗1000v * (b - r) * g * l / a * (1 / y1 + 1 / y2) * 1000

Reading the options

Now compare the form with the five options.

Option (1) has the pull on top, V(β−ρ)gLV(\beta - \rho)gL, over AA, times the sum 1Y1+1Y2\dfrac{1}{Y_1} + \dfrac{1}{Y_2}. It matches.

Option (2) has a difference. Option (3) and option (4) have the pull in the bottom. Option (5) has the moduli on top. None of these match.

Checks

Check the units. The pull V(β−ρ)gV(\beta - \rho)g is in N\text{N}. Then LA\dfrac{L}{A} is in m−1\text{m}^{-1} and 1Y\dfrac{1}{Y} is in m2 N−1\text{m}^2\,\text{N}^{-1}.

Multiply: N×m−1×m2 N−1=m\text{N} \times \text{m}^{-1} \times \text{m}^2\,\text{N}^{-1} = \text{m}. The result is a length, as it must be.

Does it make sense?

If β=ρ\beta = \rho, the upthrust holds up the whole weight, so the pull is zero and the extension is zero. The formula gives zero.

If the second rod becomes very stiff, Y2Y_2 becomes very big and 1Y2\dfrac{1}{Y_2} goes to zero. Then the first rod is the one that stretches, as the formula says.

Conclusion

e=V(β−ρ)gLA(1Y1+1Y2)e = \dfrac{V(\beta - \rho)gL}{A}\left(\dfrac{1}{Y_1} + \dfrac{1}{Y_2}\right)

The change of the length of the composite rod is V(β−ρ)gLA(1Y1+1Y2)\dfrac{V(\beta - \rho)gL}{A}\left(\dfrac{1}{Y_1} + \dfrac{1}{Y_2}\right).

The answer is (1).

The quotes give Young's modulus and Archimedes' principle. The steps T=W−UT = W - U, the same pull in the two massless rods, and the extensions adding are our reasoning from them. We take the weight of the rods as negligible, as the question says.

Teacher's note

Find the pull first: weight minus upthrust. The same pull goes through both rods. Each stretches by TLAY\dfrac{TL}{AY}, and the stretches add.

Check the units: the answer must come out in metres.

Exam tip

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