A simple pendulum consisting of a mass m and weightless string of length 1 is mounted on a support of mass M which is at

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A simple pendulum consisting of a mass m and weightless string of length 1 is mounted on a support of mass M which is at

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A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 1
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 1 (19.13 KiB) Viewed 14 times
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 2
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 2 (19.13 KiB) Viewed 14 times
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 3
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 3 (36.89 KiB) Viewed 14 times
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 4
A Simple Pendulum Consisting Of A Mass M And Weightless String Of Length 1 Is Mounted On A Support Of Mass M Which Is At 4 (30.22 KiB) Viewed 14 times
A simple pendulum consisting of a mass m and weightless string of length 1 is mounted on a support of mass M which is attached to a horizontal spring with force constant k as shown in Figure below. M www Potential Energy Reference 0 m

One of the obtained differential equations of the motion for the system is: * (m + M)x + ml cos 0 - 02) + kx - 0 (m + M)x+ ml(0 cos 0 - sin 0) + kex - 0 47 0 0 ( MM+ ml (0 cos 0 0 sin0) + kx (m+Mr+ ml cos 0 0 sin 0) + kx

The other obtained differential equation of the motion for the system is: lö + cos 0 + g sin 0 = 0 lö - * cos 0 + g sin 0 = 0 O O 10 + i cos 0 + sin 0 = 0 10 + * cos 0 + g sin 0 - 0
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