Mass, m = 14.5 kg
Length of the steel wire, l = 1.0 m
Angular velocity, ω = 2 rev / s
Cross-sectional area of the wire, a = 0.065 cm2
Let δl be the elongation of the wire when the mass is at the lowest point of its path. When the mass is placed at the position of the vertical circle, the total force on the mass is: F = mg + mlω2
= 14.5 × 9.8 + 14.5 × 1 × (2)2
= 200.1 N
\(Young's modulus = \frac{Stress }{ Strain}\)
\(Y =\frac{ \frac{F }{ A} }{ \frac{Δl }{ l} }= \frac{F \,l }{A Δl}\)
\(∴ Δl =\frac{ Fl }{ AY}\)
Young’s modulus for steel = 2 × 10 11 Pa
\(∴ Δl = \frac{200.1 × 1 }{ 0.065 × 10^{ - 4} × 2 × 10 ^{11}} = 1539.23 × 10 ^{- 7} \)
= 1.539 × 10 - 4 m
Hence, the elongation of the wire is 1.539 × 10 - 4 m.
The elastic behavior of material for linear stress and linear strain, is shown in the figure. The energy density for a linear strain of 5×10–4 is ____ kJ/m3. Assume that material is elastic up to the linear strain of 5×10–4
Two identical ball bearings in contact with each other and resting on a frictionless table are hit head-on by another ball bearing of the same mass moving initially with a speed V. If the collision is elastic, which of the following (Fig. 5.14) is a possible result after collision ?
