How can something be the cause OF something else and yet also be defined AS the change of something else?
This example is one of many that I think can show that without any direct history and future experimentation with the world, the concepts used in classical physics (and other sciences for that matter) do not really tell us anything at all. — darthbarracuda
Taking some isolated component of the formalism and asking what it really is makes no sense, at least to me. — SophistiCat
Mendel theorized that genes were the units of inheritance, but he wasn't able to observe them. That had to wait until the discovery of DNA.
Neptune was predicted based on irregularities of Uranus's orbit that could be explained by the existence of another planet.
And atoms were theorized by the ancient Greeks. It's only been in the last few decades that they've been seen, and even manipulated to produce a short animation. — Marchesk
Let us ask, “What is the meaning of the physical laws of Newton, which we write as $F=ma$? What is the meaning of force, mass, and acceleration?” Well, we can intuitively sense the meaning of mass, and we can define acceleration if we know the meaning of position and time. We shall not discuss those meanings, but shall concentrate on the new concept of force. The answer is equally simple: “If a body is accelerating, then there is a force on it.” That is what Newton’s laws say, so the most precise and beautiful definition of force imaginable might simply be to say that force is the mass of an object times the acceleration. Suppose we have a law which says that the conservation of momentum is valid if the sum of all the external forces is zero; then the question arises, “What does it mean, that the sum of all the external forces is zero?” A pleasant way to define that statement would be: “When the total momentum is a constant, then the sum of the external forces is zero.” There must be something wrong with that, because it is just not saying anything new. If we have discovered a fundamental law, which asserts that the force is equal to the mass times the acceleration, and then define the force to be the mass times the acceleration, we have found out nothing. We could also define force to mean that a moving object with no force acting on it continues to move with constant velocity in a straight line. If we then observe an object not moving in a straight line with a constant velocity, we might say that there is a force on it. Now such things certainly cannot be the content of physics, because they are definitions going in a circle. The Newtonian statement above, however, seems to be a most precise definition of force, and one that appeals to the mathematician; nevertheless, it is completely useless, because no prediction whatsoever can be made from a definition. One might sit in an armchair all day long and define words at will, but to find out what happens when two balls push against each other, or when a weight is hung on a spring, is another matter altogether, because the way the bodies behave is something completely outside any choice of definitions. — The Feynman Lectures on Physics Vol. I Ch. 12: Characteristics of Force
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