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Few other paradigms in Physics are so easy to translate into
"normal life" terms as the linear restoring force.
As a whimsical example, consider an intimate relationship
between two lovers. In this case x can represent
"emotional distance" - a difficult thing to quantify
but an easy one to imagine. There is some equilibrium
distance x0 where at least one of the lovers is most
comfortable11.11
-- this time, just to show how it works, we will not
choose x0 to be the zero position of x
but leave it in the equations explicitly.
When circumstances (usually work) force
a greater emotional distance for a while,
the lover experiences a sort of tension
that pulls him or her back closer to the beloved.
This is a perfect analogy to the linear restoring force:
What few people seem to recognize is that this "force,"
like any linear restoring force, is symmetric: it works
the same in both directions, too far apart and too close.
When circumstances permit a return to greater closeness,
the lover rushes back to the beloved (figuratively -
we are talking about emotional distance x here!)
and very often "overshoots" the equilibrium position x0
to get temporarily closer than is comfortable.
The natural repulsion that then occurs
is no cause for dismay -
you can't really have an attraction without it -
but some people seem surprised to discover that the attraction
that binds them to their beloved does not just keep acting no matter
how close they get; they are very upset that x cannot just
keep getting closer and closer without limit.11.12
In later chapters I will have much more to say about
the oscillatory pattern that gets going
[see Fig. 11.4]
when the overshoot is allowed to occur
without any friction to dissipate the energy
stored in the stretched spring [a process known as
damping]. But first I really must pick up
another essential paradigm that has been begging to be introduced.
Next: Potential Energy
Up: Captain Hooke
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Jess H. Brewer -
Last modified: Sat Nov 14 12:43:31 PST 2015