Example 1.  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_9.gif]   

Solution 1.

[Graphics:../Images/SpringMassMod_gr_10.gif]

[Graphics:../Images/SpringMassMod_gr_11.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_12.gif]


[Graphics:../Images/SpringMassMod_gr_13.gif]

 

The roots are pure complex,  [Graphics:../Images/SpringMassMod_gr_14.gif], and the natural frequencies  [Graphics:../Images/SpringMassMod_gr_15.gif],  respectively.  The general solution is formed as follows.

[Graphics:../Images/SpringMassMod_gr_16.gif]


[Graphics:../Images/SpringMassMod_gr_17.gif]

 

Aside.  The eigenfrequencies can be obtained by taking the square root of the eigenvalues of the matrix [Graphics:../Images/SpringMassMod_gr_18.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_21.gif],  respectively.

[Graphics:../Images/SpringMassMod_gr_22.gif]


[Graphics:../Images/SpringMassMod_gr_23.gif]

 

 

We can verify these solutions.  

[Graphics:../Images/SpringMassMod_gr_24.gif]


[Graphics:../Images/SpringMassMod_gr_25.gif]

 

 

[Graphics:../Images/SpringMassMod_gr_26.gif]


[Graphics:../Images/SpringMassMod_gr_27.gif]

 

 

Plot the functions  [Graphics:../Images/SpringMassMod_gr_28.gif] and  [Graphics:../Images/SpringMassMod_gr_29.gif].  In this mode of oscillation the masses are moving in opposite directions.

[Graphics:../Images/SpringMassMod_gr_30.gif]


[Graphics:../Images/SpringMassMod_gr_31.gif]

[Graphics:../Images/SpringMassMod_gr_32.gif]

 

 

Plot the functions  [Graphics:../Images/SpringMassMod_gr_33.gif] and  [Graphics:../Images/SpringMassMod_gr_34.gif].  In this mode of oscillation the masses are moving in the same directions.

[Graphics:../Images/SpringMassMod_gr_35.gif]


[Graphics:../Images/SpringMassMod_gr_36.gif]

[Graphics:../Images/SpringMassMod_gr_37.gif]

 

 

Assume that the equilibrium position along the horizontal axis is 2 and 6.  The two masses move in the opposite direction with the frequency  [Graphics:../Images/SpringMassMod_gr_38.gif], as seen in the next graph, where time is along the vertical axis.

[Graphics:../Images/SpringMassMod_gr_39.gif]


[Graphics:../Images/SpringMassMod_gr_40.gif]

[Graphics:../Images/SpringMassMod_gr_41.gif]

 

 

Assume that the equilibrium position along the horizontal axis is 2 and 6.  The two masses move in same directions with the frequency [Graphics:../Images/SpringMassMod_gr_42.gif], as seen in the next graph, where time is along the vertical axis.

[Graphics:../Images/SpringMassMod_gr_43.gif]


[Graphics:../Images/SpringMassMod_gr_44.gif]

[Graphics:../Images/SpringMassMod_gr_45.gif]

 

 

Aside.

We could plot infinitely many types of oscillation.  For illustration we plot the solution for the coefficients [Graphics:../Images/SpringMassMod_gr_46.gif].  

[Graphics:../Images/SpringMassMod_gr_47.gif]


[Graphics:../Images/SpringMassMod_gr_48.gif]

[Graphics:../Images/SpringMassMod_gr_49.gif]

 

 

[Graphics:../Images/SpringMassMod_gr_50.gif]


[Graphics:../Images/SpringMassMod_gr_51.gif]

[Graphics:../Images/SpringMassMod_gr_52.gif]

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(c) John H. Mathews 2005