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| Tags: acceleration |
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#11
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Thanks Harry, Tom & Shevek, I studied your posts carefully.
shevek wrote: Tom Roberts wrote: Ken S. Tucker wrote: Tom Roberts wrote: No. It just requires less force to accelerate a moving particle transverse to its motion compared to the force needed for the same acceleration along its motion (here all quantities are referred to a single inertial frame). That's pontification galore, care to underwrite that statement with real dynamics? The equation of motion in Minkowski spacetime for a pointlike particle of fixed mass m under the influence of 4-force F is: F = dP/d\tau P = m U where P is the particle's 4-momentum, U is its 4-velocity, and \tau is its proper time. Project this equation onto inertial coordinates {x,y,z,t} in which the particle is moving along the z axis with velocity v, and the above equation becomes: F^x = \gamma m d^2x(t)/dt^2 F^y = \gamma m d^2y(t)/dt^2 F^z = \gamma^3 m d^2z(t)/dt^2 \gamma = 1/sqrt(1-v^2) here {x(t),y(t),z(t),t} is the trajectory of the particle. As \gamma 1, it clearly requires more force for a given acceleration along the z axis than it does along either the x or y axes. Exercise for the reader: in those coordinates there is a 4th equation which I omitted. What is it? Why did I omit it? Thanks for the exercise Tom! The other equation is F^t = \gamma/c * dE/dt = \gamma/c * (F dot u) Where E is energy = m_0 \gamma c^2. I think you omitted it because this component gives information about the energy rather than the trajectory. Energy is conserved provided the force is always normal to the motion, as in the case of a charged particle in a pure magnetic field. This exercise can be done perhaps more simply without defining a proper time \tau by defining momentum in terms of the rest mass: p = \gamma * m_0 * u and then applying the product rule when taking the derivative: F = dp/dt F = \gamma * m_0 * du/dt + m_0 * u * d\gamma/dt The second term above is in the direction of the velocity, and so thus only contributes to the force component parallel to the velocity. Cheers - shevek Tom's physics comes from 1905 SR (see Principle of Relativty pg 63). While it would be fun to use the GR dU^i/ds = GAMMA^i _uv U^u U^v geodesical equation, I'd suggest a simpler scenario. Using a laser emitted from some fixed "inertial frame" accelerate an object and predict it's rate of acceleration in the inertial frame. I think that's a simple and reasonable test gedanken. My concern is a Doppler shift that does not appear in any of the equations set forth so far. Also does the transverse acceleration account for aberration. I was hoping to others realist dynamics but keep it as simple as possible. TIA Ken |
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#12
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shevek wrote:
Thanks for the exercise Tom! The other equation is F^t = \gamma/c * dE/dt = \gamma/c * (F dot u) Where E is energy = m_0 \gamma c^2. I think you omitted it because this component gives information about the energy rather than the trajectory. Energy is conserved provided the force is always normal to the motion, as in the case of a charged particle in a pure magnetic field. This exercise can be done perhaps more simply without defining a proper time \tau by defining momentum in terms of the rest mass: p = \gamma * m_0 * u and then applying the product rule when taking the derivative: F = dp/dt F = \gamma * m_0 * du/dt + m_0 * u * d\gamma/dt The second term above is in the direction of the velocity, and so thus only contributes to the force component parallel to the velocity. If a missile was propelled through an ultramundane aether which offered resistance by a factor of gamma and a booster rocket was positioned on the side of the missile, would the energy needed in the booster rocket to change the direction of the missile be less than that in the main rocket propelling the missile in the original direction? I would say yes because there is less aether resistance normal to the original direction of the missile. However, it is a bit more complicated as the motion of the missile through the aether can have a direct analogy to the motion of an object through the air. In such cases the excess pressure from the object moving forward is dissipated spherically in waves, right? Isn't that what causes the resistance? Does the math really offer an explanation of why it takes less energy to move tangentially rather than parallel? I think it has to be explained in terms of a model. In a vacuum there would be no reason for the resistance. Vern |
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#13
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#14
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Ken S. Tucker wrote: Thanks Harry, Tom & Shevek, I studied your posts carefully. shevek wrote: Tom Roberts wrote: Ken S. Tucker wrote: Tom Roberts wrote: [..] Tom's physics comes from 1905 SR (see Principle of Relativty pg 63). While it would be fun to use the GR dU^i/ds = GAMMA^i _uv U^u U^v geodesical equation, I'd suggest a simpler scenario. Using a laser emitted from some fixed "inertial frame" accelerate an object and predict it's rate of acceleration in the inertial frame. I think that's a simple and reasonable test gedanken. My concern is a Doppler shift that does not appear in any of the equations set forth so far. Hi Ken- You're right, that scenario does add more complexity. In that case, the forces on the object - one from a laboritory laser aimed parallel to the motion and one from a laboritory laser aimed perpendicular to the motion, are not equal - due to the Doppler shift as you pointed out. As the object aproaches the speed of light the longitudal laser light will be redshifted and provide less and less force. The laser will apply less and less force as the object accelerates due to the doppler effect, and in addition that force will make less and less acceleration due to the relativistic effects described. For your example the two effects (doppler + relativistic coords) combine to make the asymmetry even greater. Cheers - shevek |
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#15
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shevek wrote:
yes because there is less aether resistance normal to the original direction of the missile. However, it is a bit more complicated as the motion of the missile through the aether can have a direct analogy to the motion of an object through the air. True again. The effect is not a result of "resistance" in analogy with air restistance. There is no such thing, just as there is no air resistance for a phonon moving across the room. Rather, the effect is due to the changes in our coordinate system, which is built on light propagation and the principles of relativity. It's called viscoelasticity. With matter waves, they are perturbing virtual particles when being moved. In such cases the excess pressure from the object moving forward is dissipated spherically in waves, right? Isn't that what causes the resistance? You were right, there's no direct analogy to the motion of an object through air. That kind of aether theory has been disproven. It's called terminal velocity. With matter waves, some of the radiation is regenerated but they can only approach the driving speed. The ęther theory has not been disproven. -Aut |
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#16
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Ken, stop misspelling its, you retard.
shevek: laboritory - laboratory |
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#17
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shevek wrote:
wrote: snip If a missile was propelled through an ultramundane aether which offered resistance by a factor of gamma and a booster rocket was positioned on the side of the missile, would the energy needed in the booster rocket to change the direction of the missile be less than that in the main rocket propelling the missile in the original direction? Yes, that's what the equations above are telling us. However, if you move to the frame of the missile, you will see that the energy needed for acceleration (as measured in that frame) is the same in any direction. The affect in question (more energy needed to accelerate longitudal motion than transverse) is a coordinate-dependent effect. Right, but forget the equations for a second and consider the assumption of an ultramundane aether. In the frame where the aether is isotropic, the missile is accelerating. Since more aether resistance is encountered in the direction of the motion, more energy would be needed to accelerate the object in this frame. If you were to accelerate the object normal to the direction of motion, from the aether frame, you would only be creating a small aether resistance as the velocity w.r.t the aether in the normal direction is not nearly as much as the velocity w.r.t to the aether in the original direction. In the frame of missile, you would still find that forces were acting on the missile, a greater force coming from one direction (the direction in which in the aether frame the missile is moving) and a smaller force from normal to that direction (in which in the aether frame you were attempting to accelerate normal to the original direction). So, with the assumption of an aether, the effect is not frame dependent, it just changes from resistance against a moving object to an unknown force (or an aether wind) acting on a stationary object. Incidentally, if the missile was at rest in the ultramundane aether, and the laboratory was flying by, the observed effect would be the same. The rest frame of this unltramundane aether is non needed in the equation - hence this ultramundane aether is also superfluous as pointed out by Einstein. I'm suggesting a modification of Newton's laws to add in the effect of aether resistance and I'm suggesting that without it there is no explanation for the fact that it takes more force to accelerate an object the faster you go and to also explain why it doesn't take as much force to accelerate the object normal to its motion. I would say yes because there is less aether resistance normal to the original direction of the missile. However, it is a bit more complicated as the motion of the missile through the aether can have a direct analogy to the motion of an object through the air. True again. The effect is not a result of "resistance" in analogy with air restistance. There is no such thing, just as there is no air resistance for a phonon moving across the room. Rather, the effect is due to the changes in our coordinate system, which is built on light propagation and the principles of relativity. In this thread we're not talking about a wave, photon or phonon's resistance due to motion w.r.t a medium, but instead we are considering an object's resistance to acceleration. With the assumption of an ultramundane aether, the effect is not due to the changes in the coordinate system. In such cases the excess pressure from the object moving forward is dissipated spherically in waves, right? Isn't that what causes the resistance? You were right, there's no direct analogy to the motion of an object through air. That kind of aether theory has been disproven. I was trying to point out that there is a direct analogy between an object accelerating in an ultramundane aether and an object accelerating in the air. The Lorentz transformation formula and the Mach formula are identical and represent a condition where the faster you go the more resistance there is to the motion to infinity (or the speed of light and sound respectively). If you plot both formulas on a graph, they have identical curves. Does the math really offer an explanation of why it takes less energy to move tangentially rather than parallel? I think it has to be explained in terms of a model. In a vacuum there would be no reason for the resistance. That depends on your model of a vacuum, doesn't it. If you explain a vacuum as a kinetic distribution of space-time atoms, then describe light waves in this medium, and then build a physical coordinate system using these light waves, you should be able to expalain the different energies required for the accelerations. snip What I find interesting is that Newton seemingly assumed a vacuum for his laws of mechanics. That's understandable though because at the time there wasn't any evidence that an ultramundane aether existed and there wasn't any physical examples (like cyclotrons) to cause him to think that there would be resistance to accelerating an object (except from the mass of the object itself). But had Newton guessed that we live in a medium environment even without the air, then his laws of mechanics would have reflected resistance to motion because of the medium. IMO, Maxwell and Lorentz both understood this. Vern |
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#18
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Autymn D. C. wrote: Ken, stop misspelling its, you retard. shevek: laboritory - laboratory Thanks Autymn, I can't believe I misspelled it twice! AARGH! |
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#20
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Autymn D. C. wrote: shevek wrote: yes because there is less aether resistance normal to the original direction of the missile. However, it is a bit more complicated as the motion of the missile through the aether can have a direct analogy to the motion of an object through the air. True again. The effect is not a result of "resistance" in analogy with air restistance. There is no such thing, just as there is no air resistance for a phonon moving across the room. Rather, the effect is due to the changes in our coordinate system, which is built on light propagation and the principles of relativity. It's called viscoelasticity. With matter waves, they are perturbing virtual particles when being moved. Is this an explanation of inertia, or of relativistic mass originally under discussion? In either case, a bit more would be helpful to help us interpret your meaning. In such cases the excess pressure from the object moving forward is dissipated spherically in waves, right? Isn't that what causes the resistance? You were right, there's no direct analogy to the motion of an object through air. That kind of aether theory has been disproven. It's called terminal velocity. With matter waves, some of the radiation is regenerated but they can only approach the driving speed. The ęther theory has not been disproven. Well I apologize for saying that this kind of aether theory, or class of aether theories, has been disproven. A more accurate statement would be that experimental results are -extremely- difficult to reconcile with that type of aether theory. Again, I am talking about the kind of aether theories where the aether exists only in the space between material bodies. These theories don't make sense to me anyway, the whole point of aether is to explain force fields - and force fields certainly exist inside, and in some way are, material particles. - shev |
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