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bernhard.rothenstein
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is the use of consevation laws compulsory in relativistic dinamics?
bernhard.rothenstein said:is the use of consevation laws compulsory in relativistic dinamics?
i think the question is well-posed. the derivation can be accomplished without using the conservation laws and to show after that the derived relativistic momentum and mass comply with them.clj4 said:this is an ill-posed question, your works need to comply with conservation laws at all times (relativity or not)
Then why do you ask? Prove it.bernhard.rothenstein said:i think the question is well-posed. the derivation can be accomplished without using the conservation laws and to show after that the derived relativistic momentum and mass comply with them.
i think the question is well-posed.
is the use of consevation laws compulsory in relativistic dinamics?
The principle of conservation of energy states that energy cannot be created or destroyed, but it can be transformed from one form to another. This means that the total amount of energy in a closed system remains constant over time.
In relativistic dynamics, energy is considered to be a conserved quantity. This means that the total energy of a system, including both its kinetic and potential energy, remains constant regardless of any changes in the system.
In relativistic dynamics, momentum is also considered to be a conserved quantity. This means that the total momentum of a system, which is the product of its mass and velocity, remains constant over time.
Conservation laws, such as the conservation of energy and momentum, are necessary in relativistic dynamics to maintain the fundamental principles of the theory. These laws ensure that the fundamental properties of energy and momentum remain constant, even in the extreme conditions of relativistic speeds.
Yes, conservation laws are always applicable in relativistic dynamics. However, they may need to be modified in certain situations, such as when dealing with systems that involve mass-energy conversion or when considering the effects of gravity on energy and momentum.