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6 - N u m e r i c a l   1

Problem

A 1.50 cm length of piano wire with a diameter of 0.25 cm is stretched by attaching a 10 kg mass to one end. How far is the wire stretched?

Data

  • Length of wire, L=1.50 cm=1.50Γ—10βˆ’2 mL = 1.50 \, \mathrm{cm} = 1.50 \times 10^{-2} \, \mathrm{m}
  • Diameter of wire, D=0.25 cm=0.25Γ—10βˆ’2 mD = 0.25 \, \mathrm{cm} = 0.25 \times 10^{-2} \, \mathrm{m}
  • Radius of wire, r=D2=0.125Γ—10βˆ’2 mr = \frac{D}{2} = 0.125 \times 10^{-2} \, \mathrm{m}
  • Mass attached, m=10 kgm = 10 \, \mathrm{kg}
  • Young’s modulus for steel, Y=2.0Γ—1011 N/m2Y = 2.0 \times 10^{11} \, \mathrm{N/m}^2

To find:

  • Change in length, Ξ”L\Delta L

Prerequisite Concepts

  • Young’s modulus is defined as:
Y=FAΞ”LL Y = \frac{\frac{F}{A}}{\frac{\Delta L}{L}}

Rearranging for Ξ”L\Delta L:

Ξ”L=Fβ‹…LYβ‹…A \Delta L = \frac{F \cdot L}{Y \cdot A}
  • Force due to the weight of the mass:
F=W=mβ‹…g F = W = m \cdot g
  • Cross-sectional area of the wire (circular):
A=Ο€r2 A = \pi r^2

Solution

  1. Calculate the force applied:
F=mβ‹…g=10 kgβ‹…9.8 m/s2=98 N F = m \cdot g = 10 \, \mathrm{kg} \cdot 9.8 \, \mathrm{m/s^2} = 98 \, \mathrm{N}
  1. Calculate the cross-sectional area:
A=Ο€r2=3.14β‹…(0.125Γ—10βˆ’2)2 A = \pi r^2 = 3.14 \cdot (0.125 \times 10^{-2})^2 A=3.14β‹…1.5625Γ—10βˆ’6 m2=4.91Γ—10βˆ’6 m2 A = 3.14 \cdot 1.5625 \times 10^{-6} \, \mathrm{m^2} = 4.91 \times 10^{-6} \, \mathrm{m^2}
  1. Substitute values into the formula for Ξ”L\Delta L:
Ξ”L=Fβ‹…LYβ‹…A \Delta L = \frac{F \cdot L}{Y \cdot A} Ξ”L=98β‹…1.50Γ—10βˆ’22.0Γ—1011β‹…4.91Γ—10βˆ’6 \Delta L = \frac{98 \cdot 1.50 \times 10^{-2}}{2.0 \times 10^{11} \cdot 4.91 \times 10^{-6}} Ξ”L=1.47Γ—10βˆ’19.82Γ—105 \Delta L = \frac{1.47 \times 10^{-1}}{9.82 \times 10^5} Ξ”L=1.498Γ—10βˆ’4 m \Delta L = 1.498 \times 10^{-4} \, \mathrm{m}

Answer

The wire is stretched by Ξ”L=1.498Γ—10βˆ’4 m\Delta L = 1.498 \times 10^{-4} \, \mathrm{m} or 0.1498 mm0.1498 \, \mathrm{mm}.