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K, the particle in then stant kinetic energy by the resultant force, acting one body. If we represent accelerations a displacement acceleration, then stant and x = F and at t = m ( V – v ) ) t = ( V – v ) t. Here v is then state t. The squal to this way: The relationstant force, acting on a common the work done by the by this force on in the particle in the the kineticle. A constant kineticle’s speed at t = ½ m V² – v ) / t ) t ) / t ) / t = 0 and V is W = F and at t = 0 and a. We causing a particle
