Since the angular acceleration is equal to the ratio of torque to moment of inertia, then ε=MJ\varepsilon =\frac {M} {J}ε=JM
M=ε×JM =\varepsilon\times JM=ε×J , since J=m×R22J=\frac{m\times R^2} {2}J=2m×R2 , a m=ρ×Vm=\rho\times Vm=ρ×V , then
M=ε×ρ×V×R22M=\varepsilon\times\frac{\rho\times V \times R^2}{2}M=ε×2ρ×V×R2 =0.5×7800×(900×π4(0.52−0.22))×(0.5×0.5)22≈18091.16=0.5\times\frac{7800\times(900\times\frac{\pi}{4}(0.5^2-0.2^2))\times (0.5\times 0.5)^2}{2}\approx18091.16=0.5×27800×(900×4π(0.52−0.22))×(0.5×0.5)2≈18091.16 N×\times×m.
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