
106 Chapter 6 Springs and Spring-Like Things
Equation 5.1. If we added this, the mathematics would become considerably more
complex, for little visible improvement (remember, we’ re faking this in any case). So
we stick with the simplest kind of drag.
Solving the differential equation gives an expression for the position at any time
in the future:
p
t
=[p
0
cos(γt) +c sin(γt)]e
−
1
2
dt
where γ is a constant given by
γ =
1
2
4k −d
2
and c is a constant given by
c =
d
2γ
p
0
+
1
γ
˙
p
0
Substituting the time interval for t in the equations above as before, we can get a
value for p
t
, and calculate the acceleration required using Equation 6.5 as we did for
regular harmonic motio ...