Question 3.6: A large pendulum is composed of a 10.0 kg ball suspended by ...

A large pendulum is composed of a 10.0 kg ball suspended by an aluminum wire having a diameter of 1.00 mm and a length of 6.30 m. The aluminum is the alloy 7075-T6. Compute the elongation of the wire due to the weight of the 10 kg ball.

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Objective   Compute the elongation of the wire.

Given          Wire is aluminum alloy 7075-T6; diameter = D = 1.00 mm.

Length = L = 6.30 m; ball has a mass of 10.0 kg.

Analysis    The force on the wire is equal to the weight of the ball, which must be computed from w = m · g. Then, the stress in the wire must be checked to ensure that it is below the proportional limit. Finally, because the stress will then be known, Equation (3–8) will be used to compute the elongation of the wire.

\delta = \frac{\sigma L}{E}             (3-8)

Results       Force on the wire: F = w = m · g = (10.0 kg)(9.81 m/s2) = 98.1 N.

Axial tensile stress: σ = F/A

  A = \frac{ \pi D^{2}}{4} = \frac{ \pi(1.00  mm)^{2}}{4} = 0.785 mm²

  \sigma = \frac{F}{A} = \frac{98.1  N}{0.785  mm^{2}} = 125 MPa

Appendix A–14 lists the yield strength of 7075-T6 aluminum alloy to be 503 MPa. The stress is well below the proportional limit.

The stress can be considered to be steady for a slow-moving pendulum, and the aluminum is ductile, having 11% elongation. From Table 3–2, the design stress can be computed from

A–14  Typical properties of aluminum alloys .^{a}
Ultimate strength, s_{u} Yield strength, s_{y} Shear strength, s_{us}
Alloy and temper ksi MPa ksi MPa percent elongation ksi MPa
Alloys in wrought form
1100-H12 16 110 15 103 25 10 69
1100-H18 24 165 22 152 15 13 90
2014-0 27 186 14 97 18 18 124
2014-T4 62 427 42 290 20 38 262
2014-T6 70 483 60 414 13 42 290
3003-0 16 110 6 41 40 11 76
3003-H12 19 131 18 124 20 12 83
3003-H18 29 200 27 186 10 16 110
5154-0 35 241 17 117 27 22 152
5154-H32 39 269 30 207 15 22 152
5154-H38 48 331 39 269 10 28 193
6061-0 18 124 8 55 30 12 83
6061-T4 35 241 21 145 25 24 165
6061-T6 45 310 40 276 17 30 207
7075-0 33 228 15 103 16 22 152
7075-T6 83 572 73 503 11 48 331
Casting alloys—permanent mold castings
204.0-T4 48 331 29 200 8
206.0-T6 65 445 59 405 6
356.0-T6 41 283 30 207 10
TABLE 3–2  Design stress guidelines: Direct normal stresses.
Manner of loading Ductile material Brittle material
Static \sigma_{d} = s_{y} /2 \sigma_{d} = s_{u} /6
Repeated \sigma_{d} = s_{y} /8 \sigma_{d} = s_{u} /10
Impact or shock \sigma_{d} = s_{y} /12 \sigma_{d} = s_{u} /15

\sigma_{d} = s_{y} /2 = 503 MPa/2 = 251 MPa

Therefore, the wire is safe.

Elongation: For use in Equation (3–8), all data are known except the modulus of elasticity, E. The footnote of Appendix A–14 lists the value of E = 72 GPa = 72 × 10^{9} Pa. Then,

\delta = \frac{\sigma L}{E} = \frac {(125  MPa)(6.30  m)}{72  GPa} = \frac{(125 \times 10^{6} Pa)(6.30  m)}{72 \times 10^{9} Pa } 

\delta = 10.9 \times 10^{-3}  m =10.9 mm

Comment   What do you see around you right now that has a dimension similar to 10.9 mm (0.429 in.)? Measure the thickness of one of your fingers. Certainly, the design of the system containing the pendulum in this example problem would have to take this deflection into account.

Added Note    This problem is modeled after the “Foucault pendulum,” found in many science museums and universities. The oscillation of the pendulum allows the observation of the rotation of
the earth on its access.

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