MP is Mach's principle, which basically states that inertia (the resistance to the chnage of motion) is caused by movement relative to the background created by all the matter in the universe and therefore if we remove this matter then acceleration would be relative too and the 'fictious' inertial forces would not be present in any frames.
Hi jcsd
Thanks for the very clear and concise definition. This helps.
So inertia is resistance to change in motion, and change in motion is acceleration, so we could just say that inertia is resistance to acceleration.
MP then states the proposition that inertia, or resistance to acceleration, is caused by motion relative to the background. I have replaced your word "movement" with the word "motion," for reasons of economy of idea. {If you have no objection?)
To recap, Resistance to acceleration is caused by motion relative to the background. I have an immediate concern with the apparent lack of parity between motion, represented in physics by distance per time, and acceleration, represented by distance per (time squared). But perhaps we will return to that later.
It is the notion of background which remains to be investigated. MP, if I have it correctly, places the background at a distance from the object, as a hollow sphere surrounding the space in which the object is found, marked by certain stars of reference. Then if the marks are removed, even though the sphere might remain in place, acceleration effects disappear? This seems unsatisfactory to me. Perhaps Mach would say that it is the sphere itself which must be removed, and not merely the marked stars. Very well. Let us make it so.
Now we have an object in unmarked space. The object however has a geometry of its own, assuming it is a macroscopic agglomeration of definable points, such as an astronaut or a body of water or even two rocks on a string (or two quarks and their gluons?). Mach says it has the quality of rotation, which he says results in no accelerative forces internal to the body. His argument then seems to self-conflict, since he first says there can be no rotation in unmarked space, and then says that the body is in rotation. However, perhaps that can be overlooked, and still get some meaning from the ideas.
We have one remaining part of this problem to investigate. We have considered the object, and the space that it is in, but any observation requires a third part. That is the observer. The observer in Mach's space is an undefined entity, except that as part of Mach space, it can be assumed to be disembodied, possessing no mass or fixed position. The point of observation may be moved with no physical effect on the body or the space, as we can investigate the astronauts hand or his intestines as we will. We can recede until the object is no more than a single quantum point from our view, or we can enlarge the object and move our point of view within it until it constitutes a universe in itself.
Mach says this universe is rotating. What can that mean? Notice that he does not say that the notion of rotation is meaningless, he says that rotation produces no acceleration. Do I have this right? I am afraid I must admit I have not seen Mach's original papers, but know of these arguments only through summations by other thinkers.
If the universe is said to be rotating, I assume we must say that our observation point may take a resting position, in which its location may not have to be adjusted, and from which the various parts of the astronaut's body are seen to change in relation to each other. This change is rather specific. The astronaut is not torn apart by the motion, but remains an astronaut. Yet as we watch, we see first one side of the astronaut, then another side, and this motion repeats as the astronaut turns. We may notice that the various parts of the astronauts body move in different ways, compared to each other. There is an axis which does not seem to move, and there is a left and a right, one of which seems to move toward us, and the other away from us. If we give ourselves a sort of x-ray vision, we may see that the front side of the astronaut is moving in the opposite direction from the back side of the astronaut.
There is one other way we could see this same scene, and that is if we do not assume our point of view is in a rest position, but that our position is rotating around the astronaut, providing a series of movements and their associated viewpoints, as if we were in orbit around the astronaut's apparent axis. This is, however, not what Mach has stated. Or. perhaps, Mach would say that the two ideas of motion are equivalent.
However, I would have to disagree. The two motions, one in which we are orbiting, and the other in which the astronaut is rotating, are not the same, even in an otherwise unmarked universe. The difference has to do with the condition that our observer has to be massless and chargeless and have no effect on the object or on the universe it inhabits. The only quality our observer has is a sense of position and of direction. Maintaining a position identical to an orbital requires that our point of view take on a series of highly specific changes. This is highly complicated, requiring not only adjustments in position, but also in attitude, since we require to be looking toward the astronaut throughout our pseudo-orbit. In order to maintain such a position, we would have to do a series of extremely complicated calculations and adjustments. Fortunately for our discussion, we can just pretend that the calculations and adjustments have already been made, and we can merely state that we are in orbit around the astronaut. But if we were to actually try to simulate this motion, as in a computer animation, we would have a great deal of work cut out for us.
No, we must stick with the program given to us. We are not in motion around the astronaut. The astronaut is said to be rotating and so we must make it so, and not the other way around.
Now given that the astronaut is rotating, and the hand is moving in relation to the intestines, and the other hand is moving in a contrary direction in relation to the intestines, and yet the astronaut retains his form, is there any necessary centripetal acceleration?
We must return to the physical definition of motion and of acceleration. Motion is a change in coordinate x with respect to time. Acceleration is a change in coordinate x in relation to (time squared). I think I know what change in x is. So we must think in terms of what is meant by the difference between time and the square of time. Or more exactly, the difference between the inverse of time and the inverse of the square of time.
If an object is in simple motion, we can plot its position in the dimension x against a position in time t. The time t and the position in dimension x can be laid out on an orthogonal chart in two dimensions, with equal intervals being given to the respective time and space. Then we will see that simple motion results in a plot of a straight line.
If an object in simple motion is plotted in space against time squared, that is if the time interval is not equal but is given an exponential notation, so that the interval changes along the time line in a continuous adiabatic fashion, then we will see that the plot is not a straight line, but is curved. If the plot is a straight line on the time squared chart, we must assume that the object in motion is under some forced acceleration.
The astronaut or other macroscopic object carries with it its own referential system. We can call the length of the astronauts thumb joint an inch and the length of the astronauts foot a foot and so on, and so set up our metric for x. Then we can see if changes in x per t result in a straight line or a line that is curved. Carrying out this operation, we will find that the astronaut's hands are accelerated compared to each other, without reference to any outside conditions.
To see this, consider the position of the hands of the astronaut in a dimension x placed so that it is orthogonal, that is at ninety degrees, from the axis of rotation. When the hands are in line with the middle of the astronaut, they are moving relative to x at some velocity. However, when they are at their fullest extension in x, they are instantaneously not moving with relation to the axis at all. If we follow one hand as it moves in x, we will see that it starts out in the middle with a direction in x, reaches its extrema and stops moving instantaneously in x (we may say that it is still moving in y) and then changes direction and moves backward in x until it reaches the opposite extreme. This change in motion in x is by definition acceleration.
Have I missed anything?
I would go on from here to consider the case of a single quantum particle, because I think Mach's brilliant idea does apply to systems that are entirely local, such as may be found below the quantum foam. Quantum foam begins at about the size of a proton, 10E-9 cm, but we are aware of a continuous scale down to the Planck length of 10E-32 cm. Forgive me if I have missed the mark on the numbers a bit, but this is about the size of it.
I propose that on the Planck scale, background becomes meaningless as the ideas of space and time begin to break down. However, even on these scales, there is still geometry. Can we go on from here to consider the geometry of quarks, electrons, and the other most fundamental particles?
I am aware that quantum theorists will find this a risky business. It has been held as a common belief for almost a century now that there is no use trying to visualize qualities like spin on the quantum scale. But I think I see a way, using the ideas of Mach as modified above, to explain the measurable behaviors of quantum particles in a visual model, one which may be better than that currently in place. Would this not be a benefit to students of quantum physics? Perhaps such a model would even allow us to find answers to questions about grand unified theories, problems in cosmology, and even in other unforseen places. Or at least, better questions.
Thanks for your help. Please help me sharpen the language. The above is only a draft of an idea, and I am not really nailed to any of the terms. Have I achieved communication? Can we go on and explore this new model of quantum processes? I assure you in advance that as far as I can see, it does not contradict the findings of special or general relativity, or of the standard model of particle physics. It may, however, provide some new insight into cosmology.
Thanks,
nc