Difference between revisions of "Forest UCM Energy KEnWork"
Jump to navigation
Jump to search
Line 13: | Line 13: | ||
Consider the Kinetic Energy's temporal rate of change assuming that the mass of the particle is constant | Consider the Kinetic Energy's temporal rate of change assuming that the mass of the particle is constant | ||
− | : <math>\frac{dT}{dt} = \frac{m}{2} \frac{d}{dt}v^2</math> | + | : <math>\frac{dT}{dt} = \frac{m}{2} \frac{d}{dt}v^2= \frac{m}{2} \frac{d}{dt}\vec v \cdot \vec v</math> |
− | ::<math>= \frac{m}{2} \ | + | ::<math>= \frac{m}{2} \left (\vec \dot v \cdot \vec v + \vec v \cdot \vec \dot v \right )</math> |
[[Forest_UCM_Energy#KE_.26_Work]] | [[Forest_UCM_Energy#KE_.26_Work]] |
Revision as of 12:47, 15 September 2014
Definition of KE
For a single particle of mass m moving with a velocity v, the kinetic energy is defined as
Work Energy Theorem
Derivation
Consider the Kinetic Energy's temporal rate of change assuming that the mass of the particle is constant