9.3: Virtual Work
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We have seen that a mechanical system subject to conservative forces is in equilibrium when the derivatives of the potential energy with respect to the coordinates are zero. A method of solving such problems, therefore, is to write down an expression for the potential energy and put the derivatives equal to zero.
A very similar method is to use the principle of virtual work. In this method, we imagine that we act upon the system in such a manner as to increase one of the coordinates. We imagine, for example, what would happen if we were to stretch one of the springs, or to increase the angle between two jointed rods, or the angle that the ladder makes as it leans against the wall. We ask ourselves how much work we have to do on the system in order to increase this coordinate by a small amount. If the system starts from equilibrium, this work will be very small, and, in the limit of an infinitesimally small displacement, this “virtual work” will be zero. This method is very little different from setting the derivative of the potential energy to zero. I mention it here, however, because the concept might be useful in Chapter 13 in describing Hamilton’s variational principle.
Let’s start by doing a simple ladder problem by the method of virtual work. The usual uniform ladder of high school physics, of length
I have drawn the four forces on the ladder, namely: its weight
There are several ways of doing this, which will be familiar to many readers. The only small reminder that I will give is to point out that, if you wish to combine the two forces at the foot of the ladder into a single force acting upwards and somewhat to the left, so that there are then just three forces acting on the ladder, the three forces must act through a single point, which will be above the middle of the ladder and to the right of the point of contact with the wall. But we are interested now in solving this problem by the principle of virtual work.
Before starting, I should warn that it is important in using the principle of virtual work to be meticulously careful about signs, and in that respect I remind readers that in the differential calculus the symbols
Let us take note of the following distances:
and
If we were to increase
and
Further, if were to increase
On putting the expression for the virtual work to zero, we obtain
You should verify that this is the same answer as you get from other methods – the easiest of which is probably to take moments about E.
There is something about virtual work which reminds me of thermodynamics. The first law of thermodynamics, for example is
Let us move now to a slightly more difficult problem, which we’ll try by three different methods – including that of virtual work.
In Figure IX.5, a uniform rod AB of weight
I have marked in various angles and lengths, which can easily be determined from the geometry of the system, and I have also marked the four forces on the rod.
Let us first try a very conventional method. We know rather little about the force R of the hinge on the rod (though see below), and therefore this is a good reason for taking moments about the point A. We immediately obtain
Divide by
Now let’s try the same problem using energy conditions. We’ll take the zero of potential energy when the rod is horizontal – at which time the small mass is at a distance l below the level AC.
When the angle CAB =
The derivative is
and setting this to zero will produce the same results as before. Further differentiation (do it), or a graph of
Now let’s try it by virtual work. We are going to increase
The distance of the centre of mass of the rod below AC is
The distance of the ring below AC is
The distance BC is
Thus the virtual work is
If we put this equal to zero, we obtain the same result as before.