Example 6.  Equal Masses, Unequal spring constants.  Find the general solution to the system of D. E.'s  and plot the solution curves.

    [Graphics:Images/SpringMassMod_gr_201.gif]   

Solution 6.

[Graphics:../Images/SpringMassMod_gr_202.gif]

[Graphics:../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_204.gif]


[Graphics:../Images/SpringMassMod_gr_205.gif]

 

 

The roots are pure complex,  [Graphics:../Images/SpringMassMod_gr_206.gif], and the natural frequencies  [Graphics:../Images/SpringMassMod_gr_207.gif],  respectively.  The general solution is formed as follows.

[Graphics:../Images/SpringMassMod_gr_208.gif]


[Graphics:../Images/SpringMassMod_gr_209.gif]

 

 

Aside.  The eigenfrequencies can be obtained by taking the square root of the eigenvalues of the matrix [Graphics:../Images/SpringMassMod_gr_210.gif].





 

 

It is useful to look at the two natural modes of oscillation of the spring mass system and they exhibit the natural frequencies  [Graphics:../Images/SpringMassMod_gr_213.gif],  respectively.

[Graphics:../Images/SpringMassMod_gr_214.gif]


[Graphics:../Images/SpringMassMod_gr_215.gif]

 

 

We can verify these solutions.  

[Graphics:../Images/SpringMassMod_gr_216.gif]


[Graphics:../Images/SpringMassMod_gr_217.gif]

 

 

[Graphics:../Images/SpringMassMod_gr_218.gif]


[Graphics:../Images/SpringMassMod_gr_219.gif]

 

 

Plot the functions  [Graphics:../Images/SpringMassMod_gr_220.gif] and  [Graphics:../Images/SpringMassMod_gr_221.gif].  In this mode of oscillation the masses are moving in opposite directions.

[Graphics:../Images/SpringMassMod_gr_222.gif]


[Graphics:../Images/SpringMassMod_gr_223.gif]

[Graphics:../Images/SpringMassMod_gr_224.gif]

 

 

Plot the functions  [Graphics:../Images/SpringMassMod_gr_225.gif] and  [Graphics:../Images/SpringMassMod_gr_226.gif].  In this mode of oscillation the masses are moving in the same directions.

[Graphics:../Images/SpringMassMod_gr_227.gif]


[Graphics:../Images/SpringMassMod_gr_228.gif]

[Graphics:../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 [Graphics:../Images/SpringMassMod_gr_230.gif],
as seen in the next graph, where time is along the vertical axis.

[Graphics:../Images/SpringMassMod_gr_231.gif]


[Graphics:../Images/SpringMassMod_gr_232.gif]

[Graphics:../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 [Graphics:../Images/SpringMassMod_gr_234.gif],
as seen in the next graph, where time is along the vertical axis.

[Graphics:../Images/SpringMassMod_gr_235.gif]


[Graphics:../Images/SpringMassMod_gr_236.gif]

[Graphics:../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_238.gif].  

[Graphics:../Images/SpringMassMod_gr_239.gif]


[Graphics:../Images/SpringMassMod_gr_240.gif]

[Graphics:../Images/SpringMassMod_gr_241.gif]

 

 

[Graphics:../Images/SpringMassMod_gr_242.gif]


[Graphics:../Images/SpringMassMod_gr_243.gif]

[Graphics:../Images/SpringMassMod_gr_244.gif]

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(c) John H. Mathews 2005