Multiple Degree of Freedom Systems: Coupling of Equations of Motion
The simple two degree of freedom system we have been considering so far is shown in Figure (8.7), repeated here for convenience, for which the equations of motion were found to be
As mentioned, these equations are coupled since both and appear in each of these equations. The implication with coupled equations is that they must be solved as a system. Neither of the equations can be solved individually.
In contrast, consider the same system as above but with the central spring removed as shown in Figure 8.8. This is still a TDOF system as two coordinates are still required to completely specify the positions of the masses. The two equations of motion for this system are
and and are arbitrary constants.
* (*Note that in this case due to our choices for the system parameters. is a general result for uncoupled systems.)
As can be seen, uncoupled systems are significantly easier to solve that coupled ones. Review the effort required to obtain the solution to equations (8.20) and compare that to the effort required to obtain the solution to those in (8.21). The difference is apparent, and will become more significant as systems with more degrees of freedom are considered. It is hopefully clear from this that it is preferable to deal with uncoupled equations if possible.
Note that in matrix form, equations (8.20) and (8.21) are
respectively. As can be seen, uncoupled equations correspond to diagonal matrices (both mass and stiffness matrices must be diagonal). Any off-diagonal term leads to a coupling of the equations. In equation (8.23) the off-diagonal terms occur in the stiffness matrix, which is referred to as static coupling. The situation in which the mass matrix contains off-diagonal is termed inertia coupling. It is possible for both type of coupling to be present at the same time.
Coupling and Coordinates
For the two degree of freedom system in Figure (8.7), the equations of motion are coupled as we have seen
Consider what happens however if we look at the sum and difference of these equations:
If we now define new coordinates and as
(c) and (d) become simply
which are now uncoupled. The solutions to these equations are therefore easy to write down as
and and are the arbitrary constants. Note that we get the same natural frequencies using this representation. Further, and can be found
from and as
These can also be written as
which is exactly the same solution determined previously for this system in (8.14). Here we found the solution using only uncoupled equations in terms of the “coordinates” and . The important point of this exercise is to recognize is that
Coupling is not a property of the system. Rather coupling is a consequence of the choice of coordinates used to describe the system.
Relationship to Mode Shapes
In the linear systems we have been discussing it is (almost) always possible to find a set of coordinates which uncouples the equations of motion. That is essentially what the mode shapes represent: linear combinations of the chosen coordinates that will uncouple the equations of motion:
In the current system, which is relatively simple, we were able to “guess” that the uncoupled coordinates would be and . In general guessing like this is not very feasible. It was done here only to illustrate the concepts involved. For a general vibration problem, the uncoupled coordinates (i.e. mode shapes) can be found by following the procedure outlined earlier. This will work for (almost) all multiple degree of freedom systems.
A rigid beam (mass , length , centroidal moment of inertia ) is supported by springs at its ends as shown. Determine the equations of motion, natural frequencies and mode shapes for this system.
Solve this problem using two different sets of coordinates:
- and ,
- and ,
as illustrated below.
Be sure to identify any nodes in each mode shape.
An asymmetric machine mounting is supported by both vertical and horizontal springs as shown below.
- Using the coordinates , , and as illustrated, determine the equations of motion for this system.
- Explain how the equations of motion and mode shapes change in each of the following special cases:
- and .
The two degree of freedom system shown consists of a wheel (with mass and centroidal moment of inertia ) which rolls without slipping and a bar (with mass and centroidal moment of inertia ) connected by three springs each of stiffness .
- Using the coordinates (the horizontal position of the center of the wheel) and (the horizontal position of the lower end of the bar) show that if and , the equations of motion for this system become
- Determine the natural frequencies and mode shapes for this system.