2.41 There are mechanical, electrical, and chemical systems that are described by the same mathematics
as second-order, forced, damped harmonic motion. The resulting differential equation obtained after apply-
ing a force balance or conservation of momentum is of the form:
where x is the displacement, t is time, m is the mass, γ is the damping coefficient, k is the restoring force
(spring) constant, is the amplitude of the driving force, and ω is the frequency of the driving force.
(a) Determine the order of the ODE and whether it is linear, nonlinear, homogeneous or non homoge-
neous.
(b) Find the homogeneous solution of the ODE by hand.
(c) Find the particular solution of the ODE by hand. Find after a long time ( ). This is some-
times called the “steady state” response, even though it is actually time varying.
(d) Using MATLAB, plot the maximum amplitude of from the steady state response as a function of
the excitation frequency ω ( rad/s) for N, N/m, and kg, for three values
of γ: , , and N–s/m (three plots on the same figure). Discuss the results. What
happens at when ?
Solution
(a) The highest order derivative that appears in the ODE is second order, so this is a second order ODE.
The coefficients are all constants and the right hand side is a function only of the independent variable t, so
that this is a linear ODE. In standard form, , , , and . Therefore,
this is a non-homogeneous ODE. The given ODE is thus a second order, linear, non-homogeneous ODE.
(b) The homogeneous solution is found by setting the right hand side to zero:
md2x
dt2
——-–γdx
dt
—––kx++ A0ωt()sin=
md2x
——-–γdx
dt
—––kx++ 0=