Undergrad First order deviation from circularity

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The discussion centers on the Bertrand theorem as presented in Goldstein's "Classical Mechanics," specifically regarding the conditions for closed orbits under deviations from circularity. It clarifies that "first order deviation" refers to small deviations, which can be mathematically expressed using a Taylor series expansion. The first term of this series represents the first order term, involving the first derivative of the function at a specific point. The conversation emphasizes that closed orbits are only guaranteed for the inverse square law and Hooke's law when considering higher-order deviations. Understanding these concepts is crucial for grasping the implications of the theorem in classical mechanics.
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This is regarding the Bertrand theorem in the book Classical Mechanics by Goldstein. It is said that for more than first order deviations from circularity the orbits are closed only for inverse square law and hooke's law. What does first order deviation mean ?
 
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I think in simple words it means small deviation.

The deviation of a function ##f(x)## from its value ##f(x_0)## can be expressed as taylor series with all the powers of x.

##f(x)-f(x_0)=(x-x_0)f'(x_0)+\frac{1}{2!}(x-x_0)^2f''(x_0)+...+\frac{1}{n!}(x-x_0)^nf^{(n)}(x)+...##

The first term in this series is the first order term(because it involves first power of x and first derivative at ##x_0## ).
 
Topic about reference frames, center of rotation, postion of origin etc Comoving ref. frame is frame that is attached to moving object, does that mean, in that frame translation and rotation of object is zero, because origin and axes(x,y,z) are fixed to object? Is it same if you place origin of frame at object center of mass or at object tail? What type of comoving frame exist? What is lab frame? If we talk about center of rotation do we always need to specified from what frame we observe?

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