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 phy131studiof15:lectures:chapter12 [2015/10/10 03:25]mdawber [Properties of cross products] phy131studiof15:lectures:chapter12 [2015/10/12 09:19] (current)mdawber [Equations of motion for rotational motion] Both sides previous revision Previous revision 2015/10/12 09:19 mdawber [Equations of motion for rotational motion] 2015/10/12 09:19 mdawber [12.P.005] 2015/10/12 09:13 mdawber [12.P.008] 2015/10/12 09:13 mdawber [Equations of motion for rotational motion] 2015/10/10 03:27 mdawber [Moment of Inertia] 2015/10/10 03:25 mdawber [Properties of cross products] 2015/10/10 03:23 mdawber [Torque] 2015/10/10 03:22 mdawber [From angular to tangential quantities] 2015/10/10 03:19 mdawber [About that acceleration..] 2015/10/10 03:18 mdawber [12.P.008] 2015/10/10 03:17 mdawber [Angular acceleration] 2015/10/10 03:15 mdawber [Equations of motion for rotational motion] 2015/07/22 10:39 mdawber 2015/07/22 10:24 mdawber created Next revision Previous revision 2015/10/12 09:19 mdawber [Equations of motion for rotational motion] 2015/10/12 09:19 mdawber [12.P.005] 2015/10/12 09:13 mdawber [12.P.008] 2015/10/12 09:13 mdawber [Equations of motion for rotational motion] 2015/10/10 03:27 mdawber [Moment of Inertia] 2015/10/10 03:25 mdawber [Properties of cross products] 2015/10/10 03:23 mdawber [Torque] 2015/10/10 03:22 mdawber [From angular to tangential quantities] 2015/10/10 03:19 mdawber [About that acceleration..] 2015/10/10 03:18 mdawber [12.P.008] 2015/10/10 03:17 mdawber [Angular acceleration] 2015/10/10 03:15 mdawber [Equations of motion for rotational motion] 2015/07/22 10:39 mdawber 2015/07/22 10:24 mdawber created Line 47: Line 47: ===== 12.P.008 ===== ===== 12.P.008 ===== + ===== Equations of motion for rotational motion ===== + + At the beginning of the course we derived, using calculus, a set of equations for motion under constant acceleration. + + $v= v_{0}+at$ ​ + + $x= x_{0}+v_{0}t+\frac{1}{2}at^2$ + + $v^{2}=v_{0}^2+2a(x-x_{0})$ + + We can equally derive similar equations for our rotational quantities. Indeed as we can see that the relationships between the new rotational quantities we have now are exactly the same as those between the translational quantities we can simply rewrite the translational motion equations in terms of rotational variables. + + $\omega= \omega_{0}+\alpha t$ + + $\theta= \theta_{0}+\omega_{0}t+\frac{1}{2}\alpha t^2$ + + $\omega^{2}=\omega_{0}^2+2\alpha(\theta-\theta_{0})$ + + ===== 12.P.005 ===== ===== 12.P.026 ===== ===== 12.P.026 ===== Line 105: Line 124: - ===== Equations of motion for rotational motion ===== - At the beginning of the course we derived, using calculus, a set of equations for motion under constant acceleration. - $v= v_{0}+at$ ​ - $x= x_{0}+v_{0}t+\frac{1}{2}at^2$ - - $v^{2}=v_{0}^2+2a(x-x_{0})$ - - We can equally derive similar equations for our rotational quantities. Indeed as we can see that the relationships between the new rotational quantities we have now are exactly the same as those between the translational quantities we can simply rewrite the translational motion equations in terms of rotational variables. - - $\omega= \omega_{0}+\alpha t$ - - $\theta= \theta_{0}+\omega_{0}t+\frac{1}{2}\alpha t^2$ - - $\omega^{2}=\omega_{0}^2+2\alpha(\theta-\theta_{0})$ - - ===== 12.P.005 ===== Line 265: Line 268: We should note that the distance $R$ is the distance of each mass with respect to the axis of rotation, which need not be the center of mass, and is not an intrinsic property of an object! ​ We should note that the distance $R$ is the distance of each mass with respect to the axis of rotation, which need not be the center of mass, and is not an intrinsic property of an object! ​ + + ===== 12.P.053 ===== + ===== Two weights on a thin bar ===== ===== Two weights on a thin bar =====