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Exercises · 8.1

Q.A steel wire of length 4.7 m and cross-sectional area 3.0×10−5 m23.0 \times 10^{-5}\ \text{m}^{2} stretches by the same amount as a copper wire of length 3.5 m and cross-sectional area of 4.0×10−5 m24.0 \times 10^{-5}\ \text{m}^{2} under a given load. What is the ratio of the Young's modulus of steel to that of copper?

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This problem uses the Young's Modulus formula to relate the elongation of two wires under the same load. By equating the elongations, we find the ratio of Young's moduli for steel to copper is 1.8\boxed{1.8}.

When a material is subjected to a deforming force, it undergoes a change in shape or size. For a wire pulled along its length, this change is an elongation. Young's Modulus is a fundamental property of a material that quantifies its stiffness or resistance to elastic deformation under tensile or compressive stress. It tells us how much a material will stretch or compress when a certain force is applied.

The core idea is that stress (force per unit area) causes strain (fractional change in length). Young's Modulus (YY) is defined as the ratio of stress to strain:

Y=StressStrainY = \frac{\text{Stress}}{\text{Strain}}

For a wire of original length LL, cross-sectional area AA, subjected to a tensile force FF that causes an elongation ΔL\Delta L:

  • Stress =FA= \frac{F}{A}
  • Strain =ΔLL= \frac{\Delta L}{L}

Therefore, the formula for Young's Modulus becomes:

Y=F/AΔL/L=FLAΔLY = \frac{F/A}{\Delta L/L} = \frac{FL}{A\Delta L}

This formula is key because it connects the material property (YY) with the physical dimensions (L,AL, A) and the observed deformation (ΔL\Delta L) under a given force (FF). In this problem, we are told that both wires experience the "same amount" of stretch (ΔL\Delta L) under a "given load" (FF). This means FF and ΔL\Delta L are identical for both wires, allowing us to set up an equation to find the ratio of their Young's moduli.

  1. Identify the given information and the goal.

    We are given the following parameters for a steel wire and a copper wire:

    • Steel wire (subscript ss):
      • Length, Ls=4.7 mL_s = 4.7\ \text{m}
      • Cross-sectional area, As=3.0×10−5 m2A_s = 3.0 \times 10^{-5}\ \text{m}^2
    • Copper wire (subscript cc):
      • Length, Lc=3.5 mL_c = 3.5\ \text{m}
      • Cross-sectional area, Ac=4.0×10−5 m2A_c = 4.0 \times 10^{-5}\ \text{m}^2

    We are also told two crucial conditions:

    • Both wires stretch by the same amount: ΔLs=ΔLc=ΔL\Delta L_s = \Delta L_c = \Delta L
    • Both wires are under a given (same) load: Fs=Fc=FF_s = F_c = F

    Our goal is to find the ratio of Young's modulus of steel to that of copper, i.e., YsYc\frac{Y_s}{Y_c}.

  2. Express elongation in terms of Young's Modulus.

    From the Young's Modulus formula Y=FLAΔLY = \frac{FL}{A\Delta L}, we can rearrange it to solve for the elongation ΔL\Delta L:

ΔL=FLAY\Delta L = \frac{FL}{AY}

This equation shows that for a given force $F$, a longer wire ($L$), a smaller cross-sectional area ($A$), or a smaller Young's Modulus ($Y$) will result in a greater elongation.

3. Apply the elongation formula to both wires.

For the steel wire, the elongation is:

ΔLs=FsLsAsYs\Delta L_s = \frac{F_s L_s}{A_s Y_s}

For the copper wire, the elongation is:

ΔLc=FcLcAcYc\Delta L_c = \frac{F_c L_c}{A_c Y_c}

  1. Use the condition of equal elongation and load. Since ΔLs=ΔLc\Delta L_s = \Delta L_c and Fs=Fc=FF_s = F_c = F, we can set the two expressions for elongation equal to each other:

FLsAsYs=FLcAcYc\frac{F L_s}{A_s Y_s} = \frac{F L_c}{A_c Y_c}

The force $F$ cancels out from both sides, as it is the same for both wires:

LsAsYs=LcAcYc\frac{L_s}{A_s Y_s} = \frac{L_c}{A_c Y_c}

  1. Solve for the ratio of Young's moduli. We need to find YsYc\frac{Y_s}{Y_c}. Rearranging the equation from the previous step:

YsYc=LsAcAsLc\frac{Y_s}{Y_c} = \frac{L_s A_c}{A_s L_c}

Now, substitute the given numerical values:

YsYc=(4.7 m)×(4.0×10−5 m2)(3.0×10−5 m2)×(3.5 m)\frac{Y_s}{Y_c} = \frac{(4.7\ \text{m}) \times (4.0 \times 10^{-5}\ \text{m}^2)}{(3.0 \times 10^{-5}\ \text{m}^2) \times (3.5\ \text{m})}

Notice that the units of length (m) and area ($\text{m}^2$) cancel out, as do the powers of $10^{-5}$, leaving a dimensionless ratio, which is expected for a ratio of Young's moduli.

YsYc=4.7×4.03.0×3.5\frac{Y_s}{Y_c} = \frac{4.7 \times 4.0}{3.0 \times 3.5}

YsYc=18.810.5\frac{Y_s}{Y_c} = \frac{18.8}{10.5}

YsYc≈1.790476...\frac{Y_s}{Y_c} \approx 1.790476...

Rounding to two significant figures, consistent with the input data:

YsYc≈1.8\frac{Y_s}{Y_c} \approx 1.8

✓Final answer

The ratio of the Young's modulus of steel to that of copper is 1.8\boxed{1.8}.

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