Activity 1- Electric Field due to a Given Charge Configuration Consider the following distribution of point charges: +4.0 nC at the origin of your coordinate system (0, 0) -1.0 nC at (+lm, +1m) -1.0 nC at (+lm, -1m) 1. Make a sketch of this charge distribution on a separate piece of paper. 2. Compute the total electric field magnitude and direction at the following poin a. (+1m, 0m) b. (+1m, +2m)

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Lme eleClITC 1ielus UI tlme lmuIVidual CHarges (FTIeipie UI SuperPOSitICH).
Electric field lines are a graphical representation of the electric field. The field lines help
us understand and visualize the abstract concept of the electric field.
IN-LAB ACTIVITIES
The following activities should be completed before you leave the lab
Activity 1-Electric Field due to a Given Charge Configuration
Consider the following distribution of point charges:
+4.0 nC at the origin of your coordinate system (0, 0)
-1.0 nC at (+lm, +1m)
-1.0 nC at (+lm, -1m)
1. Make a sketch of this charge distribution on a separate piece of paper.
2. Compute the total electric field magnitude and direction at the following poin
a. (+1m, 0m)
b. (+1m, +2m)
So called to distinguish it from the charges producing the field; these are called source charges. Of
rery charge produces its own field and so acts as a source charge for others. But a charge does not
perience its own field; it cannot exert a force on itself.
1
Transcribed Image Text:Lme eleClITC 1ielus UI tlme lmuIVidual CHarges (FTIeipie UI SuperPOSitICH). Electric field lines are a graphical representation of the electric field. The field lines help us understand and visualize the abstract concept of the electric field. IN-LAB ACTIVITIES The following activities should be completed before you leave the lab Activity 1-Electric Field due to a Given Charge Configuration Consider the following distribution of point charges: +4.0 nC at the origin of your coordinate system (0, 0) -1.0 nC at (+lm, +1m) -1.0 nC at (+lm, -1m) 1. Make a sketch of this charge distribution on a separate piece of paper. 2. Compute the total electric field magnitude and direction at the following poin a. (+1m, 0m) b. (+1m, +2m) So called to distinguish it from the charges producing the field; these are called source charges. Of rery charge produces its own field and so acts as a source charge for others. But a charge does not perience its own field; it cannot exert a force on itself. 1
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