Dynamics 2e 477
Problem 3.46
The force on the mass for the device in Prob. 3.43 and the force on the mass in the Duffing equation
obtained from the device equation of motion (and defined by Eqs. (2) and (3)) can be plotted as a function
of
x
. The nature of that force depends on whether or not the springs are initially stretched (
L>L
0
) or
initially compressed (
L<L
0
). The figure shows the elastic restoring force on the mass
m
as a function of
the displacement xfor four different cases:
Force for device with LD2and L0D1.
Force for device with LD1and L0D2.
Force for the Duffing equation with LD2and L0D1.
Force for the Duffing equation with LD1and L0D2.
For small
x
, the force given by the Duffing equation is a good approximation to the force in the device.
Explain which of the curves corresponds to a “hardening” spring (a spring that gets stiffer as you pull
it) and which corresponds to a “softening” spring (a spring that gets less stiff as you pull it), and explain
physically why we see this behavior.
Solution
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