Physics 201- Introduction to Electricity & Magnetism
September 6- Visualizing & Calculating Electric Fields

 

 

 

 
 

 

  Multiple Charges & Continuous Charge Distributions
 

As you might guess from the electric field definition, fields are just like forces in that they can be added.  You just have to remember that they are both vectors.

If we have a bunch of point charges we would simply add up the field due to each point charge at the location of interest.
 
 






Consider the point charges becoming even smaller and more numerous.  Then this summation becomes an integral.  (Remember integrals are nothing more than summations of really small objects.)
 
 








Depending on how the charges are distributed, we make have a 1-D integral (line distribution), 2-D integral (surface distribution) or 3-D integral (solid distribution)
 

To get everything in terms of a common variable, so we can integrate, we transform the small chunk of charge (dq) to look like the charge density * a small volume chunk.
 
 
Common notation for charge density 
SI Units of charge density
 "Small volume chunk" (with Cartesian version) 
"Small chunk of charge"
Point charge
q
C
     
Line charge distribution (1-D)
l
C/ m
dl = dx
dq = l dl
Surface charge distribution (2-D)
s
C/ m2
dA = dx dy
dq = s dA
Volume charge distribution (3-D)
r
C/ m3
dv = dx dy dz
dq = r dv

 
 

 

About the Course
Syllabus
Schedule
Study Hints
Problem Solving
Contract
Homework- assignments & solutions
Miscellaneous links
About Dr. Jeff
Feedback


 
 
 
 
 

 

 
     
Jeff Phillips
phillips@lmu.edu
Loyola Marymount University
Fall 2002