Linear Impulse and Momentum for a Particle in a Plane   Click here to skip to Impact.    

 

 

Key Concept:  The principle of linear impulse and momentum for a particle is just an integrated

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

from  F = ma.

 

 

In a Nut Shell:  The principle of linear impulse and momentum for a particle is that the linear

impulse acting on the particle equals its change in linear momentum during the time of the

impulse, say from t1 to t2.

 

 

                                        t2                   

                                        ∫ Σ F dt  =  m v2  -  m v1  

                                        t1

 

Principle of Linear Impulse and Momentum for a Particle

                       

NOTE:  The principle of linear impulse and momentum is a vector equation.     

                i.e.  It has x and y components. 

 

                                            

Meaning of terms:

 

  t2 

  ∫ Σ F dt  = the linear impulse acting on the body from  t1 to  t2 

  t1

 

Σ F = ΣFx i + ΣFy j  =  sum of all external forces acting on the particle

 

m v2  = linear momentum of the particle at time t2

 

m v1  = linear momentum of the particle at time t1

 

 

Strategy:

 

Step 1:  Draw a free body diagram showing all external forces acting on the particle.  Note that

not all forces acting on the particle may result in a change in its linear momentum.

 

Step 2:  Calculate the linear impulse and set it equal to the change in linear momentum of the        

              particle

 

 

Click here for examples.   

 


   Return to Notes on Dynamics


Copyright © 2019 Richard C. Coddington
All rights reserved.