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 3
Homework Statement
Attached.
Homework Equations
I am assuming the coordinate transformation is [itex] \vec{x}' = \vec{x} + \alpha\vec{\gamma} [/itex] ?
Then you have [itex] \vec{v}' = \vec{v} + \alpha\frac{d\vec{\gamma}}{dt} [/itex]
And r is the magnitude of the x vector.
The Attempt at a Solution
Part A.
So to get the change in lagrangian, I put the primed v and x into the Lagrangian and subtracted the given lagrangian to get:
[tex] \Delta L = \frac{1}{2}m\vec{v} + \alpha\frac{d\vec{\gamma}}{dt}^2 + \frac{k}{\vec{x} + \alpha\vec{\gamma}}  \frac{1}{2}mv^2  \frac{k}{r} [/tex]
So following examples from class, I expand the vector magnitude terms and neglected the second order alpha quantity, which leaves me with
[tex] \Delta L = \frac{1}{2}m(2\alpha \vec{v} \cdot \frac{d\vec{\gamma}}{dt}) + \frac{k}{\sqrt{\vec{x}^2 + 2 \vec{x}\cdot\alpha\vec{\gamma}}}  \frac{k}{r} [/tex]
So I thought maybe to taylor expand the first k/r term up to first order alpha, after factoring out [itex] \vec{x}^2 [/itex]. And since x is r, i can cancel out the last k/r term. That leaves me with
[tex] \Delta L = m(\alpha \vec{v} \cdot \frac{d\vec{\gamma}}{dt})  \frac{k\alpha}{\vec{x}^3}(\vec{x}\cdot\vec{\gamma}) [/tex]
Now taking the derivative of gamma, and noting that dn/dt should be zero and that p cross dx/dt and dp/dt cross x should also be zero, I get for the final expression, plugging everything in
[tex] \Delta L = m\alpha[\vec{v} \cdot [\frac{d\vec{x}}{dt}\times( \vec{p}\times\hat{n}) + \vec{x} \times (\frac{d\vec{p}}{dt} \times \hat{n})]]  \frac{k\alpha}{\vec{x}^3} [\vec{x} \cdot [\hat{n} \times (\vec{p} \times \vec{x}) + \vec{x} \times (\vec{p} \times \hat{n})]] [/tex]
But from here, I don't really see how I could get it to equal part b, or if I even did the right process, I probably made a mistake in getting the difference, any tips?
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