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A pendulum consists of point mass m on the end of a rigid massless rod of length

ID: 3897633 • Letter: A

Question

A pendulum consists of point mass m on the end of a rigid massless rod of length b. The other end of the rod is attached to point mass M that is free to move along a frictionless, horizontal surface. The origin is on the surface (see diagram), and we set U(0) = 0. As generalized coordinates: use theta (the angle between the pendulum bar and the vertical) and X (the distance from M to the origin). At t = 0: M is at the origin (X = 0)moving at vo; theta=theta_o, and theta'_o =0.

Assume mass M is slowly increasing, according to M = Mo + kt, where k is a small positive constant and t is time in seconds. Use the same generalized coordinates theta and X.

a) i. Write the Lagrangian for this system of two masses.
ii. Write the Euler-Lagrange equations for this system. Simplify, but
DO NOT SOLVE!


b) Without further calculations: answer each question YES or NO, and support your answer.

i. Is ETOT = H?
ii. Is H(amiltonian) conserved?

iii. Is ETOT conserved?

Explanation / Answer

To write the Lagrangeian all is identical with your first problem EXCEPT the kinetic energy of mass M

Ek(M) = (M0+k*t)*(X_dot)^2 /2


the total Lagrangeian is

L = (M+m+kt)*(X_dot)^2 /2 + m*b^2*(theta_dot)^2 /2 - m*g*b*cos(theta)


Observation: this lagrangeian DOES depend on the time explicitly


dL/dX = 0

dL/d(X_dot) =(M+m+kt)*(X_dot)

d/dt (dL/d(X_dot)) = d/dt [(M+m+kt)*(X_dot)] = k*(X_dot) +(M+m+kt)*(X_dot_dot)


First Euler Lagrange equation is

dL/dX = d/dt (dL/d(X_dot))

0 = k*(X_dot) +(M+m+kt)*(X_dot_dot)




dL/d(theta) = m*g*b*sin(theta)

dL/d(theta_dot) = m*b^2*(theta_dot)

d/dt (dL/d(theta_dot)) =m*b^2*d/dt (theta_dot) = m*b^2*(theta_dot_dot)


Second Euler lagrange Equation is

dL/d(theta) = d/dt (dL/d(theta_dot))

g*sin(theta) = b*(theta_dot_dot)


b)

i) L = T-U does depend on time t explictly. Therefore H is different from Etot.

ii) H = T+U does depend on the time t explicitly. Therefore H is not conserved.

iii) There are no external forces that act on the system except the conservative force of gravity on mass m. Therefore the total energy Etot is conserved.




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