Virtual Work and Displacements
Using the concept of virtual displacements, and virtual work, we can derive the equations of motion of lumped parameter systems.
Example 1 Mass/Spring System
Here number of degrees of freedom =1 Co-ordinate to describe the motion is x Now consider free-body diagram, at some time t
General one degree of freedom system If q1 is the co-ordinate used to describe the movement then the general form of δW is as follows:
we call δq1 - generalised displacement Q1 - generalised force. From principle of virtual work
Example Referring to the mass/spring system again
x= q1
Example 2
Simple pendulum
This is another one degree of freedom system. During a virtual displacement, δθ, the virtual work done is
Example 3 - two degrees of freedom system
| 1. What is virtual work? | ![]() |
| 2. How is virtual work related to displacements? | ![]() |
| 3. How is virtual work different from actual work? | ![]() |
| 4. What are the applications of virtual work in engineering? | ![]() |
| 5. How is virtual work used in the field of physics? | ![]() |