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You're better to find some way to post it here.Feynmanisthegoat said:Ya man I am sorry this is my first post so I don't know what went wrong but it's figure 16.4 from the Feynman lectures on physics.
Momentum conservation in special relativity is a fundamental principle that states that the total momentum of a closed system remains constant, regardless of any internal changes or interactions within the system.
In special relativity, the concept of momentum is extended to include not only the mass and velocity of an object, but also its energy. This means that the total momentum of a system is conserved not just in terms of linear momentum, but also in terms of relativistic momentum.
Momentum conservation is important in special relativity because it is a fundamental law of nature that helps us understand and predict the behavior of particles and systems at high speeds and energies. It also plays a crucial role in many important phenomena, such as particle collisions and nuclear reactions.
One example is the decay of a particle into two or more particles, where the total momentum of the initial particle is conserved in the momenta of the resulting particles. Another example is the collision of two particles, where the total momentum of the system is conserved before and after the collision.
In classical mechanics, momentum conservation only applies to closed systems at low speeds. In special relativity, momentum conservation applies to all systems, including those at high speeds and energies. Additionally, in special relativity, momentum is conserved in terms of both linear and relativistic momentum, whereas in classical mechanics, only linear momentum is conserved.