Problem 1: Recall the two-mass system from a previous problem set, in which you deter- mined the (stable) equilibrium point of the system. (a) Let y be the distance of the bead from the ceiling. From the earlier problem, rewrite U(0) so that the potential energy is a function of this variable y, instead of 0. Also, given the expression for the equilibrium angle, find the equilibrium position yo for this system. (b) Expand U(y) in a Taylor series around Yo to show that for small oscillations, U(y) can be written in the Hooke's Law form ky², and determine the "effective spring constant" k. (c) Write the total kinetic energy T of the system as a function of y. Compare your kinetic and potential energy for this system to the energy expressions in the SHO, and determine this system's angular frequency for small oscillations. M b Ꮎ m

International Edition---engineering Mechanics: Statics, 4th Edition
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Chapter10: Virtual Work And Potential Energy
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Problem 10.56P: The stiffness of the ideal spring that is compressed by the slider C is k = 250 N/m. The spring is...
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Problem 1: Recall the two-mass system from a previous problem set, in which you deter-
mined the (stable) equilibrium point of the system. (a) Let y be the distance of the bead
from the ceiling. From the earlier problem, rewrite U(0) so that the potential energy is a
function of this variable y, instead of 0. Also, given the expression for the equilibrium angle,
find the equilibrium position yo for this system. (b) Expand U(y) in a Taylor series around
yo to show that for small oscillations, U(y) can be written in the Hooke's Law form ky²,
and determine the "effective spring constant" k. (c) Write the total kinetic energy T of the
system as a function of y. Compare your kinetic and potential energy for this system to
the energy expressions in the SHO, and determine this system's angular frequency for small
oscillations.
M
b
Ꮎ
m
Transcribed Image Text:Problem 1: Recall the two-mass system from a previous problem set, in which you deter- mined the (stable) equilibrium point of the system. (a) Let y be the distance of the bead from the ceiling. From the earlier problem, rewrite U(0) so that the potential energy is a function of this variable y, instead of 0. Also, given the expression for the equilibrium angle, find the equilibrium position yo for this system. (b) Expand U(y) in a Taylor series around yo to show that for small oscillations, U(y) can be written in the Hooke's Law form ky², and determine the "effective spring constant" k. (c) Write the total kinetic energy T of the system as a function of y. Compare your kinetic and potential energy for this system to the energy expressions in the SHO, and determine this system's angular frequency for small oscillations. M b Ꮎ m
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