The work-energy theorem relates the change in kinetic energy of a particle to the work done on it by an external force: AK = W = [ F dx. Writing Newton's second law as F = dp/dt, show that W = Jv dp and integrate by parts using the relativistic momentum to obtain %3D %3D %3D
The work-energy theorem relates the change in kinetic energy of a particle to the work done on it by an external force: AK = W = [ F dx. Writing Newton's second law as F = dp/dt, show that W = Jv dp and integrate by parts using the relativistic momentum to obtain %3D %3D %3D
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![2. The work-energy theorem relates the change in kinetic energy of a particle to the
work done on it by an external force: AK = W = J F dx. Writing Newton's second law
as F = dp/dt, show that W = Jv dp and integrate by parts
using the relativistic momentum to obtain
mc2
mc
K =
VI - v/c²
|](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F577768b7-2319-4884-a404-40e6ac8608b5%2F9350c820-dd96-4f90-908a-401bd5079830%2F6qo7ey_processed.jpeg&w=3840&q=75)
Transcribed Image Text:2. The work-energy theorem relates the change in kinetic energy of a particle to the
work done on it by an external force: AK = W = J F dx. Writing Newton's second law
as F = dp/dt, show that W = Jv dp and integrate by parts
using the relativistic momentum to obtain
mc2
mc
K =
VI - v/c²
|
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