Why does a force not do any work if it's perpendicular to the motion?

As explained by SchrodingersCat, mathematically work is proportional to the scalar product of force and line element. Therefore any forces acting perpendicular to the path do not contribute to the work.

Now you might want to ask why work is defined like this. I would like to justify this definition taking your example of the moon.

In physics work is intimately related to energy: basically if you want to change the energy of an object you need to do work on it. Now in the case of the moon there are two relevant energies, (1) kinetic energy of the moon related to the magnitude (but not direction) of the moon's velocity, i.e. its speed; and (2) gravitational energy related to the position of the moon in the earth's gravitational field; this one depends on the distance moon-earth.

For (1), since perpendicular forces do not change the magnitude of velocity (only their direction), the perpendicular force should not enter into the equation of work (since it does not contribute to the energy change).

For (2) if you displace the moon always perpendicular to the direction of the gravitational force, you stay at the same distance, i.e. at the same gravitational potential energy. Therefore such perpendicular displacements do not change the energy and should not enter in the expression for work.

Actually, work or, "work" as we mean in physics, has been mathematically defined as $$W=\int_{x_1}^{x_2}\vec F\cdot d\vec{s}$$ So if $\vec{F}$ and $d\vec{s}$ are orthogonal vectors, that is, the angle between the vectors is $90^\circ$, then according to the above formula, no work is done, physically; in this case, by the earth on the moon.

As @SchrodingersCat explained, there will be no work on the system if the force is orthogonal to the displacement. However, I would like to elaborate the answer a little further.

What is the physical meaning of representing work done on a body by the dot product of the force and displacement of the object?

Because an object can move even without a force (Newton's first law says about this), the motion however will be an unaccelerated one. So a body could displace even if there is no force. If you have studied classical mechanics, you may have heard that it is the linear momentum which is the generator of translation, not force.
To say a work is to be done by a force on the object, it should have some effect on the object, right? Any dynamical property (like in this case, the effect of a force) is represented by a change in position coordinate of the object (the order of which varies according to the dynamical quantity) w.r.t time, because position is the fundamental quantity in dynamics.
If the force has some effect on the object (which is acceleration, of course), then this force contributes some displacement along the direction of applied force (even if there is motion already in some other direction). In such a case, the effect of force on the body can be measured by taking the component of the resultant (or net, if you insist) displacement along the direction of the applied force. So, work done by a force is defined as the product of the applied force with the displacement component caused by this force. This can be achieved by taking the dot product of the the two vectors-Force and the net displacement.

So, what does it mean no work is done if force and displacement are orthogonal?

In Euclidean geometry, orthogonal vectors implies mutually perpendicular vectors. However, the actual sense is that the two vectors are independent. This means that one has no common component with the other, which according to the above discussions states that one vector has no effect on the other. So, the displacement occurred is not due to the force given. Geometrically, that is possible only of force and displacement are perpendicular so that their dot product vanishes. This is why there is no work done on the system if the applied force and the resultant displacement are perpendicular.

As others have mentioned, work (in 3D) on a system in defined as the dot product between the force on the system and its displacement. If they are perpendicular, no work is done.

In terms of intuition, what it means is that the force "redirects" the system (the moon, in your case) but in such as way that some of the particles are sped up and some are slowed down in the redirecting such that the net result is that the total energy of the moon is the same as it was earlier. The moon is forced to move in a circular, but in such a way that its energy remains the same at every point (at least, in the extremely simple model that you are assuming).

Background

The basic physics principle regarding the energy of a system is that the energy changes when work is done on the system, or the system does work on a different system. The work can either increase (positive work) or decrease (negative work) the total energy of the system.

Forces are the agents of work. Only external forces can change the total energy of a system. Internal forces cause exchanges of energy between pieces of the system.

Let's consider a system, the Moon (only). The gravitational pull of the Earth can do work on the system. That would change the total energy of the Moon, which in this case would simply be a change in kinetic energy. What does a change of kinetic energy mean? It means that the speed of the object has changed.

The Moon

If the Moon is moving in a circular orbit, then the instantaneous velocity of the Moon is always perpendicular to the instantaneous acceleration, so according to the (correct) definition of work in other answers, $$W=\int \vec{F}\cdot\mathrm{d}\vec{s},$$ the work is zero.

Your Question

You have asked

Why is there no work done if support force is perpendicular to the motion?

That is, what is the physics behavior that says the perpendicular force doesn't change the energy?

Because the change in energy (by work being done) is a change in the kinetic energy, the force must change the speed of the objects in the system. Accelerations which are perpendicular to the instantneous velocity only change the direction, not the speed. In order to change the speed there must be a component of acceleration which is not perpendicular.

An aside on potential energy

Potential energy is a system energy. If your system is the Moon only, there is no gravitational potential energy. If your system is the Earth and Moon, then one can consider the gravitational energy due to the interaction of the two. But when accounting for work, it's an either/or situation: Either you measure energy as the sum of kinetic and potential, or you consider kinetic only, modified by the work done by the gravitational interaction. You cannot count both simultaneously, because a potential energy change is defined as the negative of the work done by a conservative force (in this case, gravitational), when relative positions of the interacting objects change.

I think you are right @Shrodingers cat. It would be better to clarify the answer this way.

Work done (w) = F . d

                         = F d Cos θ

At 90 degrees, θ = 90 and Cos 90 = 0,

W = F x d x Cos 90

= F x d x 0 = 0 Joule.

So, when the force is applied perpendicularly to the surface, the work done will be zero.

I see that most of the posters have answered this question in terms of the usual definition of work. That's fine as far as it goes, but to many people the definition of work seems somewhat arbitrary in the first place.

An alternative would be to treat the work-energy theorem $$W_\text{net} = \Delta T \;,$$ (with $T$ the kinetic energy) as an expected behavior (because it is integral in building the conservation law from Newtonian principles and the conservation principle is so useful) and use that to deduce the form that work must take and thus show the reason for the scalar product.

What follows is just an outline.

• The straight-line version gives us $W_\parallel = F_\text{net} \,\Delta x$.
• Uniform circular motion shows us that speed (and therefore kinetic energy) are not changed by forces perpendicular to the direction of motion. That is $W_\perp = 0$.
• We may then break any net force into its parallel and perpendicular components and note that the work comes wholly from the parallel one so that writing the work in terms of the scalar product becomes a natural step.

This also leads us to the main physical content of that definition: forces applied perpendicularly to the direction of motion don't chnage the speed of the object and are in that way different from forces applied along (or against) the direction of motion.

At a higher level of sophistication one would employ Noether's theorem as a postulate and work from there.