Check out the field patterns displayed in this video.

https://www.youtube.com/watch?v=63FnT0W-Hxc

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Electic Field  |  Field Patterns

Charge Distribution Field Patterns

The electric field from a distribution of charge, like that on a charged rod, is fundamentally a superposition of all the fields from the individual charges. Electric fields add by the principle of superposition, which is to say they add linearly and like all other vectors we've learned about.

This is an image of two positively charged ions of different charges and vector arrows of the two different electric charge fields of the ions and it is also broken up into x and y components. There is also another vector showing the resultant field or the net electric field.                    $\overrightarrow{E}_{net} = \sum \overrightarrow{E}_i$

Sometimes the physics representation of a field is presented in the form of Field Lines, where the strength of the field is larger where the lines are more closely spaced. In the field line representation, field lines start at positive charges and end on negative charges. The diagram below is the eletric field for a dipole.

This is an image of an electric field of a positively charged and negatively charged ion. It shows the positively charged ion showing an electric field pointing out of the ion and a negatively charged ion showing an electric field pointing towards the ion.

Through superposition, the net field for a number of charge distributions can be determined. It's interesting to note that the electric field for a zero dimensional charge (a point charge) falls off like 1/r2 - the field for a one dimensional line of charge falls off like 1/r - and the field from a two dimensional sheet of charge doesn't fall off at all. It's no coincidence that as you increase the dimensions of the charge distribution, the field decreases how fast it falls off.

This is an image of different electric fields of three positively charged shapes. The first shows a positively charged sphere called a point charge with vector arrows pointing out from the sphere in all directions where the electric field is proportional to one divided by the radius squared. The second shows a rod of positive charge called an infinite line of charge with the electric field pointing out from the rod and the electric field is proportional to one over the radius. The third shows a infinite plane of charge with the electric field only pointing either up or down from the plane and the electric field is proportional to one. The units of the electric field vector is in units of Newtons divided by Coulombs.

The Electric Field due to an Infinite Sheet of Total Charge $Q$

$|\overrightarrow{E}_{net}| = \frac{Q}{2 \epsilon_0 A}$,      where $\epsilon_{0} = 8.85 x 10^{-12} F \cdot m^{-1}$, and $A$ is the area of the sheet.

If the sheet is infinite or you are close to a finite sheet, the field doesn't even decrease with increased distance. As you move further away from the plate, the electric fields from charges further and further away start to add more constructively, causing the field to remain constant. Putting two plates separated by some distance, with opposite charges, is called a Parallel Plate Capacitor. The fields inside the plates are uniform and provide an excellent tool for studying electric fields. 

Key Equations and Infographics

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OpenStax Reading


OpenStax Section 18.7  |  Conductors and Electric Fields in Static Equilibrium

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OpenStax Section 18.8  |  Applications of Electrostatics

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Check out the field patterns displayed in this video.

https://www.youtube.com/watch?v=63FnT0W-Hxc

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Practice

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Fundamental examples

(1) What is the magnitude of the Electric field at a location $r = 2 \hspace{0.2 cm} nm$ from a point charge with charge $q=10 \hspace{0.2 cm}nC$ that is located at the origin?

(2) Three point charges $q_1 = q_2 = q_3 = 5 \hspace{0.2 cm}nC$ are placed equidistant from each other on the x-axis: $q_1$ is located at $x= -2 \hspace{0.2 cm}nm$, $q_2$ is located at the origin, and $q_3$ is located at $x = 2 \hspace{0.2 cm} nm$. A point charge $q_4 = 1\hspace{0.2 cm} nC$ is placed on the y-axis, 2 namometers up from the origin. (a) What is the magnitude of the electric force that $q_4$ feels? (b) What is the direction of the electric force on $q_4$? (c) What is the direction of the electric force if $q_4 = -1 \hspace{0.2 cm}nC$ instead?

(3) A point charge $q_1 = -20 \hspace{0.2 cm}nC$ is located at a position $r_1 = <-3,0> \hspace{0.2 cm}nm$. (a) What is the magnitude of the electric field at point $r_a = <0, 3> \hspace{0.2 cm}nm$. (b) By what factor does the magnitude of the electric field at point $r_a$ decrease if another point charge with magnitude $q_2 = 20 \hspace{0.2 cm}nC$ is placed at the origin? (c) Calculate the magnitude and direction of the force that a point charge with magnitude $q_3 = -1 \hspace{0.2 cm}nC$ would feel if it were placed at position $r_a$ for both cases (a) and (b). [Optional (d) What is the electric force on $q_3$ if charge $q_1$ is removed?]

(4) (More time-consuming - practice with computing the electric field from multiple source charges in an arbitrary configuration) Three point charges $q_1 = 5 \hspace{0.2 cm}nC$, $q_2 = 10 \hspace{0.2 cm}nC$, and $q_3 = -2 \hspace{0.2 cm}nC$ are placed as follows: $q_1$ is located at $r_1 = <- 3,0> \hspace{0.2 cm}nm$, $q_2$ is located at $r_2 = <0,0> \hspace{0.2 cm}nm$, and $q_3$ is located at $r_3 = <1, 2> \hspace{0.2 cm}nm$. (a) What is the magnitude and direction of the electric field at point $r_p = <8, 8> \hspace{0.2 cm}nm? 

 

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Practice Problems

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Recommended example practice problems 

  • *OpenStax, has practice problems at the end of every section
  • PhysicsClassroom, 27 problems on charge and the electric field, Website Link
  • University of Greenbay: Guided problem on the electric force, Website Link

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