The work energy theorem is useful however for solving problems in which the net work is done on a particle by external forces is easily computed and in which we are interested in finding the particles speed at certain positions of even more significance is the work energy theorem as a starting point for a broad generalization of the concept.
Work energy theorem examples.
Work energy theorem holds for both positive and negative work done if the work done is positive then final ke increases by amount of the work and if work done is negative then final ke decreases by the amount of work done example 1.
W g w n w f k f k i.
A brief overview of energy kinetic energy gravitational potential energy and the work energy theorem for algebra based physics students.
For example consider the following figure according to work energy theorem work done by all the forces change in kinetic energy.
Equation for the work energy theorem the most commonly encountered form of the theorem is probably wnet 1 2 mv2 1 2 mv02 where v0 and v are the initial and final velocities of the object and m is its mass and wnet is the net work or total work.
The term work is used in everyday life quite frequently and we understand that it s an act of doing something.
The work energy theorem explains the reasons behind this physics of no work.
For example you are working right now on your grasp of physics by reading this article.
We know that all the car s kinetic energy is lost to friction.
This definition can be extended to rigid bodies by defining the work of the torque and rotational kinetic energy.
W n work done by a normal.
We apply the work energy theorem.
Therefore we first need to determine the car s kinetic energy at the moment of braking using.
In fact the building of the pyramids in ancient egypt is an example of storing energy in a system by doing work on the system.
The principle of work and kinetic energy also known as the work energy theorem states that the work done by the sum of all forces acting on a particle equals the change in the kinetic energy of the particle.
But physics itself might not agree on this.
Where w g work done by gravity.
For example when a ball is held above the ground and then dropped the work done by the gravitational force on the ball as it falls is equal to the weight of the ball a force multiplied by the distance to the ground a displacement.
Some of the energy imparted to the stone blocks in lifting them during construction of the pyramids remains in the stone earth system and has the potential to do work.