| hypothesis of the motion due to a shift of the center of mass of isolated systems |
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| Written by Сергей Макухин | |
| Friday, 02 May 2008 | |
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Transferred via translate.google.com
Notorious theorem of teormeha said that the isolated system can not remove the very material bodies themselves, as is always performed in pairs and the third law of Newton, as well as the law of conservation of energy. But times change, and this theorem can be qualitatively extended ... Suppose there is a certain length of the shaft at its ends are located on the wheel (the same mass) but different moments of inertia. By the middle of the source (energy) revolution of the shaft with the flywheel. As can be seen from the above system is completely symmetrical about its mass center of mass. So, the first phase of the system is fixed (center of mass is strictly in the middle). The second phase includes a source (energy) revolution. The system acquires the same angular velocity (another mass which repel it acquires a rotation in the other side - it should not be considered because it does not change the position of the center of mass system as a whole). Let us ask that, in this case happens to the location of the center of mass of the system? Because the flywheels at the ends of the shaft (same mass) are different moments of inertia, the energy of rotation will be different. Recall that the energy of rotation is the product of moment of inertia at the angular velocity squared divided by two. In our case, the flywheel with a large moment of inertia becomes large kinetic energy of rotation, hence the mass. That is, there was asymmetry of the masses of the system to its center, as well as energy divided by the speed of light squared is the same weight. You can take the other largest masses and moments of inertia, and other location source (energy) revolution of the shaft. This movement involves a revolving cycle Makhovikov with the information that would leave their total energy at the point of convergence, after which everything is repeated again and again. Quite another picture is observed in the new case. If, as stated, was first on the shaft (the end) are on the wheel of equal weight but varying the moment of inertia, and they can only rotate at its ends, but does not move along on it. Introduce more additional terms. Flywheels can transmit its time of one another across the field (which we include, at a time when we need). And at the beginning (first stage) only rotates the flywheel with a large moment of inertia. Center of mass system is defined. The second phase, we include a field, and it transmits the rotation of wheel with a smaller moment of inertia. This occurs on the third law of dynamics for the rotation. In this case, the kinetic energy of rotation will move in the direction of wheel with a smaller moment of inertia, which again confirms the location of the new mass asymmetry on the initial center of mass - and a new center of mass will shift to the flywheel with a lower moment of inertia. So, the hypothesis made on the center of mass displacement of an isolated system - I found it necessary to share with the readers of these reasons - I hope that you will appreciate how this is justified The material is protected |