A steel rod of length 2000cm and uniform cross sectional area 3×10^3cm2 at 28°C. Find the change in length and the force due to exerted by the rod
(Linear expansivity of steel=1.2×10^-5/K
Young's modulus of steel = 2.0×10^7/N/cm2
We use the definition for the tensile stress "F\/A" required to keep the rod’s length constant, then we find the force exerted with the Young's modulus (Y), the linear expansivity of steel ("\\alpha"), the change of temperature as "\\Delta T =T-T_0=(28-20)\u00b0C=8\u00b0C=8\\,K", and the cross-section area (A):
"\\frac{F}{A} = -Y\\alpha \\Delta T \\implies F =-YA\\alpha \\Delta T\n\\\\ F =-(2\\times10^{7}\\frac{N}{cm^2})(3\\times 10^3\\,cm^2)(1.2\\times10^{-5}\\,K^{-1})(8\\,K)\n\\\\ F =-5.76\\times10^{6}\\,N"
The change in length of the rod can be found with the relations for the thermal and tension fractional changes:
"(\\frac{\\Delta L }{L_0})_{thermal} = \\alpha \\Delta T\n\\\\ \\implies \\Delta L_{thermal} =\\alpha \\Delta T L_0=...\n\\\\ ...= (1.2\\times10^{-5}K^{-1})(8K)(2000\\,cm)\n\\\\ \\therefore \\Delta L_{thermal} =0.192\\,cm\n\\\\ (\\frac{\\Delta L }{L_0})_{tension} = \\frac{F}{AY}=-(\\frac{\\Delta L }{L_0})_{thermal}\n\\\\ \\therefore \\Delta L_{tension} =-\\,0.192\\,cm"
In conclusion, we find that the change in length is "\\Delta L_{tension}=-0.192\\,cm", and the force exerted by the rod as "F=-5.76\\times 10^{6}\\,N" (F<0 because it is a compressive force on the steel rod).
Reference:
Comments
Leave a comment