Example 6. Equal Masses, Unequal spring constants. Find the general solution to the system of D. E.'s and plot the solution curves.
Solution 6.
![[Graphics:../Images/SpringMassMod_gr_203.gif]](../Images/SpringMassMod_gr_203.gif)
Put the D.E.'s in operator form and eliminate y to obtain a fourth order D.E. for x, and find the roots of its characteristic equation.
![[Graphics:../Images/SpringMassMod_gr_205.gif]](../Images/SpringMassMod_gr_205.gif)
The roots are pure complex,
,
and the natural frequencies
, respectively. The
general solution is formed as follows.
![[Graphics:../Images/SpringMassMod_gr_209.gif]](../Images/SpringMassMod_gr_209.gif)
Aside. The
eigenfrequencies
can be obtained by taking the square root of the eigenvalues of the
matrix
.
It is useful to look at the two natural modes of oscillation of
the spring mass system and they exhibit the natural
frequencies
, respectively.
![[Graphics:../Images/SpringMassMod_gr_215.gif]](../Images/SpringMassMod_gr_215.gif)
We can verify these solutions.
![[Graphics:../Images/SpringMassMod_gr_217.gif]](../Images/SpringMassMod_gr_217.gif)
![[Graphics:../Images/SpringMassMod_gr_219.gif]](../Images/SpringMassMod_gr_219.gif)
Plot the functions
and
. In
this mode of oscillation the masses are moving in opposite
directions.
![[Graphics:../Images/SpringMassMod_gr_223.gif]](../Images/SpringMassMod_gr_223.gif)
![[Graphics:../Images/SpringMassMod_gr_224.gif]](../Images/SpringMassMod_gr_224.gif)
Plot the functions
and
. In
this mode of oscillation the masses are moving in the same
directions.
![[Graphics:../Images/SpringMassMod_gr_228.gif]](../Images/SpringMassMod_gr_228.gif)
![[Graphics:../Images/SpringMassMod_gr_229.gif]](../Images/SpringMassMod_gr_229.gif)
Assume that the equilibrium position along the horizontal axis is
2 and 6. The two masses move in the same direction with
the frequency
,
as seen in the next graph, where time is along the vertical axis.
![[Graphics:../Images/SpringMassMod_gr_232.gif]](../Images/SpringMassMod_gr_232.gif)
![[Graphics:../Images/SpringMassMod_gr_233.gif]](../Images/SpringMassMod_gr_233.gif)
Assume that the equilibrium position along the horizontal axis is
2 and 6. The two masses move in opposite directions with
the frequency
,
as seen in the next graph, where time is along the vertical axis.
![[Graphics:../Images/SpringMassMod_gr_236.gif]](../Images/SpringMassMod_gr_236.gif)
![[Graphics:../Images/SpringMassMod_gr_237.gif]](../Images/SpringMassMod_gr_237.gif)
Aside.
We could plot infinitely many types of oscillation. For
illustration we plot the solution for the coefficients
.
![[Graphics:../Images/SpringMassMod_gr_240.gif]](../Images/SpringMassMod_gr_240.gif)
![[Graphics:../Images/SpringMassMod_gr_241.gif]](../Images/SpringMassMod_gr_241.gif)
![[Graphics:../Images/SpringMassMod_gr_243.gif]](../Images/SpringMassMod_gr_243.gif)
![[Graphics:../Images/SpringMassMod_gr_244.gif]](../Images/SpringMassMod_gr_244.gif)
(c) John H. Mathews 2005