The Contact Force of Solids and Fluids

56. The particles of fluids are moved with equal force towards all particles

A hard body existing in a fluid can be determined to move by the smallest force.

We do not perceive the particles of fluids moving because they are too small. But their movement is easily inferred from their effects, especially in air and water, due to the fact that many other bodies disturb them.

This is because no bodily action, such as this corruption, can occur without local motion.

The causes of their motion will be discussed below.

The difficulty with fluids is in their particles not being able to all be moved to any one part at the same time.

This uniform movement would be necessary to allow the motion of bodies coming from any direction, as we see that they do not hinder it.

For example, the solid body B moves towards C.

• Particles of the intermediate fluid D are carried in the opposite direction from C towards B.
• These will not aid its motion but will rather hinder it more than if they were completely at rest.

To resolve this difficulty, it must be remembered that:

• rest is contrary to motion, not motion
• the direction of motion towards one part is contrary to the direction of motion towards the opposite part

Likewise, everything that moves always tends to continue in a straight line.

So while the solid body B is at rest, the opposition of the particles of the fluid body D is greater against it than it were if it were moving.

There are as many particles of D moving from C towards B as there are moving from B towards C.

• They are the same particles that, coming from C, impinge on the surface of body B, and then are turned back towards C.

Each of these, considered separately, when it strikes B, pushes it towards F.

• Thus, it impedes it from moving towards C than if they were at rest.

However, since just as many tend from F towards B and push it towards C, B is not pushed more towards one side than the other.

Therefore, unless something else intervenes, remains immobile.

Whatever shape B has, it will always be accurately pushed towards one side by as many particles of the fluid, but not towards the others.

We must assume that B is surrounded on all sides by the fluid DF.

If the quantity of this fluid is not as great in F as in D, it does not matter. This is because it does not act on B as a whole, but only on those parts of it that touch its surface.

So far, we have considered B as immobile.

Now we assume that it is pushed towards C by some force to combine with the particles of the fluid DF, and to direct them to push towards C, and to communicate to it a part of their motion.

57. Demonstration of the same thing.

The hard body B is not yet in the fluid FD.

But the particles of this fluid are arranged in a ring-like fashion, moving circularly according to the order of the noted AEIOU and likewise for OUY.

For a body to be fluid, its particles must move in multiple ways, as previously mentioned.

Now, let the hard body B rest in this fluid FD between A and O. What will happen?

The AEIO particles will be prevented from passing from O to A to complete the circle of their motion.

Similarly, the OUYA particles will be prevented from going from A to O.

• Those coming from I towards O will push B towards C.
• Those coming from Y towards A will push it equally towards F.

Hence, they alone will not have the force to move it.

But they will be reflected:

• from O to U
• from A to E.

This will result in one circulation from the two, following the order of the noted AEIOUYA.

And so, due to the encounter with body B, their motion will not be halted in any way.

Only the determination will change. They will not proceed in lines as straight or as close to straight as if they did not collide with B.

Assume some new force pushes B towards C.

It will combine with the force from the fluid particles coming from I towards O to push B towards C.

• This will overcome the force from Y towards A which pushed B towards F.

Therefore, it will suffice to change their determination and make them move according to the order of AEIOUYA, as required to not hinder the motion of body B.

What I say here about the AEIOUY particles also applies to all the other particles of the fluid FD that collide with B.

Each of them, among those pushing it towards C, is opposed by an equal number of others pushing it in the opposite direction, and that the very small force added to them is sufficient to change their determination.

Although they may not perhaps describe such circles as represented here by AEIO and OUY, undoubtedly they all move circularly and in some ways equivalent to this.