Formally, a kinetic energy is any term in a system's Lagrangian which includes a derivative with respect to time.
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Formally, a kinetic energy is any term in a system's Lagrangian which includes a derivative with respect to time.
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Standard unit of kinetic energy is the joule, while the English unit of kinetic energy is the foot-pound.
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Kinetic energy can be transferred between objects and transformed into other kinds of energy.
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For example, a cyclist uses chemical Kinetic energy provided by food to accelerate a bicycle to a chosen speed.
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The chemical energy has been converted into kinetic energy, the energy of motion, but the process is not completely efficient and produces heat within the cyclist.
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The kinetic energy has now largely been converted to gravitational potential energy that can be released by freewheeling down the other side of the hill.
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The Kinetic energy is not destroyed; it has only been converted to another form by friction.
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In inelastic collisions, kinetic energy is dissipated in various forms of energy, such as heat, sound and binding energy .
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Several mathematical descriptions of kinetic energy exist that describe it in the appropriate physical situation.
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Translational kinetic energy, that is the kinetic energy associated with rectilinear motion, of a rigid body with constant mass, whose center of mass is moving in a straight line with speed, as seen above is equal to.
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When discussing movements of a macroscopic body, the kinetic energy referred to is usually that of the macroscopic movement only.
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The kinetic energy of the system in the center of momentum frame is a quantity that is invariant .
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At a low speed, the relativistic kinetic energy is approximated well by the classical kinetic energy.
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So, the total energy can be partitioned into the rest mass energy plus the Newtonian kinetic energy at low speeds.
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Kinetic energy can be expressed as the total energy minus the rest energy:.
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For one particle of mass m, the kinetic energy operator appears as a term in the Hamiltonian and is defined in terms of the more fundamental momentum operator.
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