Principle of Work and Energy for Particles in a Plane                

 

 

Key Concept:  The principle of work and energy for a particle is just an integrated form of

Euler's First Law by integrating  F and ma with respect to displacement instead of just starting

from  F = ma.

 

 

In a Nut Shell:  The principle of work and energy for a particle in a plane is that the work

done on the particle from position 1 to position 2 equals its change in kinetic energy from position 1 to position 2. 

W1-2  =  T2  -  T1

Principle of Work and Energy for a Particle

where

 

W1-2 = the work by all forces acting on the particle that actually do work in going from 

            position 1 to  position 2

 

 T2  =  the total kinetic energy of the particle in position 2

 T1  =  the total kinetic energy of the particle in position 1

 

Note that both work and kinetic energy are scalar quantities (not vectors).

 

 

The key steps in applying the Principle of Work and Energy are as follows:

 

 

Step 1:  Draw a free body diagram showing all external forces and moments acting on

the particle.  Note that not all forces acting on the particle may actually do work.

 

 

Step 2:  Calculate the work done in going from position 1 to position 2.  Common forces

include those due to gravity, applied loads, friction, and spring loading.

 

 

Step 3:  Calculate the kinetic energy of the particle in position 1 and in position 2.

The kinetic energy for a particle (center of mass of a body) results from translation only.

 

 

Total Kinetic Energy:      T  =  ½ mv2  (ft lb or N m)

 

where   m = mass of particle ,  v  =  speed of the particle    ½ mv2  =  kinetic energy of the particle 

                      

Work done by a spring    W1-2 = ½ k ( di2 – df2)    (ft lb or N m)

 

where   k = spring constant, (lb/ft, N/m)   di = the initial extension of the spring, (ft, m) and

                                                                   df = the final extension of the spring (ft, m)

Click here for examples.

 



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