Constant central force
This simulation explores the non-Newtonian potential V(r) = kr,
in terms of the mechanical energy E, for k, L > 0, in
dimensionless units:
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The unit mass m is the particle mass (or the reduced mass for
the 2-body system).
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The unit length is the radius of the circular orbit: r0
= (L2/mk)1/3.
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The unit time is mr02/L.
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In these units we have m = L = k = 1.
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On the left appears in red the effective
potential energy r+1/2r2:
its maximum is located at the point (r,E) = (1,3/2). You
may use the mouse (or the controls below) to select the mechanical
energy E and the initial polar distance r.
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Particle's plane motion (or the relative motion in the 2-body problem)
is displayed on the right. You may use the mouse to select the initial
position: the program will automatically set r.
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Put the mouse pointer over an element to get the corresponding tooltip.
Activities
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Try different values for r and E to check that, although
all orbits are bounded, most of them are not periodic, as predicted by
Bertrand's theorem.
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However, the theorem does not preclude isolated periodic orbits. In
fact, (apart from the circular orbit for E = 3/2) it is not
that difficult to find some of them.Try near the following values: E
= 1.7, 2.4, 3.05.
This is an English translation of the Basque original for a course
on mechanics, oscillations and waves.
It requires Java
1.5 or newer and was created by Juan
M. Aguirregabiria with Easy
Java Simulations (Ejs) by Francisco
Esquembre. I thank Wolfgang Christian and Francisco Esquembre for
their help.