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Please explain where the angular velocity squared comes from in 1d) and thoroughly explain 1d) thanks!

1) In the deepest, darkest reaches of space. far, far away from the influence of other matter and matters of civilization, in. (10 points) Find the mechanical energy of the system in this inertial frame of reference as a function of the separation di

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Answer #1

See, from the equation given above in b) we have calculated r​​​​​​1​​​ & r​​​​​​2 , so now

In order to find the velocity of each block in inertial frame, (taken as centre of mass of the system, since it is un-accelerated)

We use V​​​​​​1 = \omega *r​​​​​​1 & V​​​​​​2 = \omega *r​​​​​​2

And finally when we want to calculate total energy, we are required to add kinetic (K) as well as potential energy (U) of the system.

K = (0.5)*m​​​​​​1*(V​​​​​​1)2 + (0.5)*m​​​​​​2*(V​​​​​​2)2

K = (0.5)*m​​​​​​1*\omega2*(r​​​​​​1)2 + (0.5)*m​​​​​​2*\omega2*(r​​​​​​2)2

Now substituting, values of r​​​​​​1 & r​​​​​​2, we get

K = (0.5)*{m​​​​​​1*m​​​​​​2/(m​​​​​​1+m​​​​​​2)}*(\omega*R)2

And the potential energy of the system is given by the spring potential energy which is given by { E = (0.5)*k*x​​​​​​2​​​}

Where k is spring constant, and x is the extension in the spring

We can see from the diagram, that extension in spring is (R-L​​​​o)

Hence U = (0.5)*k*(R-L​​​​o)2

Now, finally substituting \omega ,

We know both the particles are performing circular motion, hence the spring force provides the centripetal force

Hence,

m1*\omega2*r1 = k*(R-L​​​​o)

Using value of r​​​​​​1 ,

m​​​​​​1*\omega2*(R*m​​​​2/(m​1 + m​​​​​​2)) = k*(R-L​​​​o)

Hence we get, \omega 2 = {(m​​​​​​1+m​​​​​​2)*k*(R-L​​​​o)}/(m​​​​​​1*m​​​​​​2*R)

Finally substituting \omega 2,

We get the final results as given in answer in d) part.

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