Virtual Work

By Mallesham Devasane|Updated : January 11th, 2017

Virtual displacement: Given a system in equilibrium, its virtual displacement is imagined as follows: Move the system slightly away from its equilibrium position arbitrarily but consistent with the constraints. This represents a virtual displacement of the system.

Virtual displacement is denoted by Virtual-Work_files (1) to distinguish it from a real displacement Virtual-Work_files (2).

Virtual work: The work done by any force Virtual-Work_files (3) during a virtual displacement is called virtual work. It is denoted by Virtual-Work_files (4). Thus

Virtual-Work_files (5)

Work done by a constraint force is usually zero, implies that virtual work done by a constraint force is also zero. Also keep in mind that in calculating the work Virtual-Work_files (6) done by the force Virtual-Work_files (7) represents the displacement of the point where the force is being applied.

Principle of virtual work: The necessary and sufficient condition for equilibrium of a mechanical system without friction is that the virtual work done by the externally applied forces is zero.

For a system in equilibrium, each particle in the system is in equilibrium under the influence of externally applied forces and the forces of constraints.

For the ith particle:

Virtual-Work_files (8)

For a system of composed of many subsystems:

Virtual-Work_files (9)

Net virtual work done by constraint forces is zero. This means that the total virtual work done by the external forces vanishes.

Virtual-Work_files (10)

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