Classical Mechanics, Coupled Harmonic motion

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SUMMARY

The discussion focuses on setting up the equations of motion for a coupled harmonic motion system involving two springs with relaxed lengths l1 and l2. The solution separates the problem into center of mass motion and internal motion described by coordinates x1 and x2. The equations derived include the center of mass position r_{13} and the forces acting on the blocks, leading to the formulation of normal modes of vibration. The suggested approach emphasizes using the form Ce^pt for the solutions after accounting for the center of mass motion.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with harmonic oscillators and normal modes
  • Knowledge of coupled systems in classical mechanics
  • Ability to manipulate differential equations
NEXT STEPS
  • Study the derivation of normal modes in coupled oscillators
  • Learn about the center of mass motion in multi-body systems
  • Explore the application of differential equations in mechanical systems
  • Investigate the effects of spring constants on oscillation frequencies
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Students and educators in physics, particularly those focusing on classical mechanics and oscillatory motion, as well as anyone preparing for exams involving coupled harmonic systems.

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Homework Statement



Set up the equations of motion for the system shown in Fig. 4.16. The relaxed lengths of
the two springs are l1, l2 . Separate the problem into two problems, one involving the motion
of the center of mass, and the other involving the "internal motion" described by the two
coordinates x1, x2. Find the normal modes of vibration.

Homework Equations


Figure 4.16 is attached

The Attempt at a Solution



The problem is already turned in and we have a test tomorrow but here is the general outline of my solution. So the center of mass of blocks 1 and 3 is

r_{13}= xm_3+(x-l_1-x_1)m_1

and using Newton's law, and the fact that the force on this subsystem is -k_2x_2, we have

(m_1+m_2)\ddot r_{13}= m_3\ddot x+(\ddot x-\ddot x_1)m_1=-k_2x_2

and similarly with the system 2-3

the total force on just block 3 is easy so we have these three equations, assume x, x_1, and x_2 all have the form Ce^pt for DIFFERENT constants C. Substitute and solve for p.

Main question: are the equations I outlined above correct?
 

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The variables are x,x_1,x_2 so I would define each of them to be positive going towards the right. You haven't done that, so it makes it a bit more confusing, but still technically correct.

You should try the form Ce^pt only after you have taken away the motion of the centre of mass. (I'm guessing you knew that, but they might give you marks for saying it explicitly, so you should probably say it).
 

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