Reference Frame Fragments


I've written a lot of stuff on reference frames and inertial frame. Here I collect fragments that are superceded or junk, just in case I ever want to use them again.

Fragments:

  1. From an IAL 1, probably all superceded, but I'd better have a scan through it when I've got the new inertial frame basics written.
    1. In frames of reference NOT in free fall, there are locally observable/apparent/noticeable mass-dependent forces.

      The mass-dependent forces are

      1. gravity.
      2. inertial forces due to accelerations relative to the local free-fall frame that would be right where you are if there were NO mass-dependent forces. Inertial forces are sometimes called fictitious forces, but yours truly deprecates that term since they act exactly like gravity for all local observations---exactly. That they act exactly so is an axiom of general relativity.
      3. The cosmological constant force or the dark energy force. One or the other seems to exist, but they are only important on the large cosmological scale and NOT on smaller scales.

      To be precise, the mass-dependent forces are all linearly dependent on the mass of an object in a force field. Only gravity has a special name for its force field: i.e., the gravitational field.

      Mass-dependent forces are subclass of body forces.

    2. As aforesaid, all reference frames local (i.e., at the same place or nearly enough at the same place) as an inertial frame and NOT accelerated with respect to it are also inertial frames.

    3. The out-of-date concept of inertial frames was due to Isaac Newton (1643--1727) who posited there was one fundamental inertial frame which he called absolute space.

      The fixed stars were on average at rest in absolute space.

      All reference frames unaccelerated with respect to absolute space were also exact inertial frames.

      All other reference frames could only be approximate inertial frames.

      and all the old celestial mechanics practitioners from his day until general relativity (discovered 1915) actually knew that free-fall frames acted just like exact inertial frames or their calculations would never have been correct.

      What they did and what we still do (because it is exactly right to do it) is just take the center of mass (see subsection Center of Mass below) of an astronomical object in free fall and that use that center of mass as the origin of an inertial frame for the calculation of the motions of the parts of the astronomical object.

      Note when we say an astronomical object is in free fall, we almost always mean that its center of mass is in free fall in the force field of mass-dependent forces due to external astronomical objects.

      Usually, the force field is just the gravitational field.

      The astronomical objects could be pressure-supported astronomical objects (e.g., planets or stars) or kinetic energy-supported astronomical objects (e.g., planet-moon systems, planetary systems, star clusters, galaxies, galaxy clusters).

      Why is this procedure exactly right. Because general relativity tells us free-fall frames are exact inertial frames.

    4. Also general relativity tells there is NO singular fundamental inertial frame like absolute space.

      General relativity plus modern cosmology tells us there is a continuum of fundamental inertial frames defined by points that participate in the mean expansion of the universe. These inertial frames are called comoving frames. We consider comoving frames in IAL 30: Cosmology.

      But there are lots more inertial frames since all free-fall frames are exact inertial frames.

    5. A key point about inertial frames is they do NOT rotate with respect to each other and with respect to the bulk mass-energy of the observable universe.

      So there is NO absolute space, but there is absolute rotation: i.e., rotation with respect to the bulk mass-energy of the observable universe (see also Wikipedia: Inertial frame of reference: General relativity).

      This absolute rotation is usually just assumed understood without bothering to explicate what one means.

      But there may be exceptions to absolute rotation just described. In very strong gravitational fields (like very near black holes) maybe inertial frames do rotate with respect to the bulk mass-energy of the observable universe???---but yours truly has to guess about this since no one explicates this factoid.

    6. Nowadays for very accurate/precise measurements of of absolute rotation, we make measurements relative to cosmologically remote quasars and galaxies (see Wikipedia: International Celestial Reference Frame).

      For somewhat less accurate/precise, but usually adequate, measurements of absolute rotation, we use the fixed stars (which in traditional meaning used by yours truly are just the naked-eye stars). The system of fixed stars has a very low absolute rotation and is effectively zero for most purposes.

    7. Rotating frames are tricky because they actually form a continuum of reference frames each of which can be considered for a sufficiently short time as an inertial frame.

      But that treatment is very inconvenient

      So special inertial forces have been devised to ????? UNDER RECONSTRUCTION BELOW ?????

      In fact, at location on the surface of the Earth, one can ignore inertial forces to good approximation for most purposes---but NOT all purposes.

      ????? UNDER RECONSTRUCTION BELOW ?????

    8. In our discussion, when we say free-fall frame (or inertial frame), we almost always mean (without saying) a reference frame attached to a physical object to avoid the obscurities of discussing one NOT so attached.

    9. Free-fall frames are reference frames are acted on by a uniform external gravitational field ONLY ideally.

      That is why they are free-falling.

      If other forces act on the reference frame, then the reference frame CANNOT be exactly a free-fall frame---but it might be approximately one for some purposes---like any location on the surface of the Earth.

      Other forces include, e.g., the pressure force, the normal force (i.e., a rigid body force), and the electromagnetic force.

      If these other forces cause small enough accelerations, then a reference frame, may be approximately a free-fall frame for some purposes.

      Note that a uniform external gravitational field does NOT include gravitational fields internal to the reference frame which are just treated as causing internal gravitational forces.

      Note also a uniform external gravitational field is actually caused by everything in the universe external to the reference frame---as far as we know.

      Note moveover that a uniform external gravitational field is an ideal limit that is approached as the reference frame becomes small compared to the size scale over which the external gravitational field varies.

    10. All physical theories are referenced to inertial frames, except general relativity (GR) and, maybe in a sense, thermodynamics. General relativity (discovered 1915), in fact, told us that inertial frames are free-fall frames---they were a bit mysterious before that.

    11. All inertial frames in the observable universe do NOT rotate with respect to each other, except maybe in super strong gravitational fields like near black holes????. No reference yours truly knows of spits out the exception factoid, but yours truly guesses it is so.

      In fact, we can say the observable universe (i.e., its average behavior) defines the absolutely non-rotating frame for us.

    12. The fundamental inertial frames are the continuum of comoving frames that participate in the mean expansion of the universe.

      The expansion of the universe (meaning the expansion of the observable universe) is a scaling up of space WITHOUT any twisting which is consistent with our saying the observable universe (i.e., its average behavior) defines the absolutely non-rotating frame for us.

    13. Besides the comoving frames, there are many other inertial frames since all free-fall frames are inertial frames.

    14. Any reference frame accelerating relative to a local (i.e., at the same place) inertial frame is a non-inertial frame.

    15. If you are in non-inertial frame defined by a rigid body (e.g., a car turning a sharp corner or an accelerating rocket) mysterious "body forces" seem to be throwing you around and pushing you into the rigid body. Actually, you are just trying to move in a straight line at a constant speed per Newton's 1st law of motion and the rigid body must exert a real contact force on you to accelerate you with the rigid body---which can sometimes be unpleasant.

      The mysterious "body forces" are NOT real forces, but they sure act like real body forces. They are called inertial forces) and are used as trick to treat non-inertial frames as if they were inertial frames.

    16. Now we are NOT in free fall on the surface of the Earth. Why can we treat the ground wherever we are as defining an inertial frame? The center of the Earth (which is its center of mass) is in free fall---so it defines an inertial frame. We accelerate relative to this inertial frame because of the Earth's rotation. (Note any change of direction from straight line is an acceleration in Newtonian physics.) But this rotation is in a sense slow: the rotational period is a day. So the non-inertial frame effects of being in a rotating reference frame are small for most purposes.

    17. Note rotating frames are in general NOT inertial frames.

      For important example, consider a rigid rotator: the bits of it at any radius are NOT in free fall (NOT moving under the gravitation force ONLY) and they are rotating relative to the observable universe which inertial frames do NOT do.

      Now the center of mass of an orbiting astro-body does define inertial frame---when that point is NOT taken as rotating relative to the observable universe per usual.

      The surfaces of orbiting astro-bodies are in general NOT inertial frames because they are rotating relative to the observable universe, except in very rare cases.

      But the surface locations may be approximately inertial frames just as the surface locations on the Earth are if their acceleration relative a local (i.e., at the same place) inertial frame is sufficiently small.

      Note that a Earth surface location is in rotation around the Earth's axis, but that rotation NOT an orbit around the Earth's axis because it is NOT caused by gravity ONLY, but by gravity and the normal force of the ground.

      Another complication for being on the surface of the Earth is that external gravitational field on the Earth is NOT uniform over the Earth. But this effect is also small for most purposes.

      So for most purposes, we can treat every location on the surface of the Earth as being an inertial frame.

      The same is true for the surface locations, mutatis mutandis, of almost all planets or stars.

    18. But we CANNOT treat a location on the surface of the Earth as being an inertial frame for all purposes.

      Weather and long-range artillery are affected by non-inertial frame effects which are treated by using inertial forces. Note these phenomena have noticeable non-inertial frame effects because they have such a large size scale compared to most human scale activities.

      You can notice non-inertial frame effects on a small scale by special equipment: e.g., Foucault pendulum (see the figure below: local link / general link: pendulum_foucault.html).

    In the following sections, we elaborate on the above points elaborately.

    The very next section, takes up some salient features of Newtonian physics.

  2. Also from IAL 1 and probably superceded, but a scan through it is needed.

  3. Inertial Frames:

    Inertial frames of reference are reference frames with a physical nature.

    They are essential for understanding all of physics even though high-school presentations of physics often gloss over them.

    We explicate inertial frames in the multi-image figure below (local link / general link: frame_inertial_free_fall.html)

    See the figure below (local link / general link: alpine_tundra.html) for a picturesque zone of the rotating reference frame of the surface of the Earth that can be treated as inertial frame for many purposes.

    We consider non-inertial-frame effects on the surface of the Earth at some length below in subsection Inertial Forces on the Earth's Surface

  4. A figure that needs condensation:


  5. Yet another figure that that needs reworking.