Students will estimate the work done by a given electric field. They will connect the work done to the height of a plastic surface graph of the electric potential.
What Students Learn:
- Students practice doing a vector line integral of an electric field.
- Students match the electric field to a surface representing the potential and see that a positive line integral of the electric field corresponds to a drop in the potential (a negative change) \(\int \vec{E} \cdot \vec{dr} = -\Delta V\)
Time Estimate: 20 min
Introduction
- Students should have practice with doing vector line integrals. We suggest the Vector Integrals activity as a warmup.
- Students should know that the electric field in the negative gradient of the electric potential.
Whole Class Discussion / Wrap Up:
- Emphasize the “Chop, Multiply, Add” approach to doing the vector line integral. Allow several groups to share how they performed the integral.
- Talk about how since the electric field is the gradient (slope) of the potential, the line integral corresponds to multiplying the slope by the “run” to get the “rise”.
- But there is an overall negative sign, so a positive slope corresponds to a “drop”.
Estimate Work on A Path: The attached vector field represents an electric field. Draw a path starting at the red star and ending at the purple triangle. Estimate the work done on a test charge by the field along the path you drew. The longest vector shown on the vector field has a magnitude of \(15\) electric field units.
Prep - change the beginning and end points to vary the level of difficulty of the integration as needed.
Strategies we've seen:
- Chop, Multiply, & Add (what we most want) Select a path tangent to the electric field, chop up the path, estimate the distance between points and magnitudes of electric fields, multiply, and add.
- Estimation with Average Value Estimate an average electric field along the path, estimate the length of the path, and multiply.
- Change in Potential (Incorrect) Finding the change in potential by saying that the lengths of the arrows are the values of the potential.
Be on the lookout: - Students do not attend to units. This is a good place to discuss how distance on the vector map can mean physical distance or electric field magnitude.
Units: We have intentionally left off SI units for electric field. For electric field, students can either use N/C, which helps students to think about the electric field as force per charge, or V/m, which helps students to think about the electric field as the gradient of the potential. Discussing both is useful.
Path Independence: Some students have trouble distinguishing the path independence of the work done by a conservative field and the path independence of the total displacement. These students will argue that the work done on two different paths is the same because the total displacement is the same. It is nice to have a non-conservative field on hand to give to these students to demonstrate that, although the displacement is path independent, the work is not always path independent.
Relate Representations: How is the work done by the electric field related to the surface?
Discussion: This is a good place to talk about how the electric field is the gradient(slope) of the surface. You're multiplying the slope by a “run” to get a “rise”.
Discussion: Most students know that electric field vectors point toward negative charges and that the negative charge lies at the bottom of a potential well. However, most students are really surprised by the negative sign here. This is the big bang for this activity.
group Small Group Activity
30 min.
group Small Group Activity
30 min.
group Small Group Activity
30 min.
coulomb's law electric field charge ring symmetry integral power series superposition
Students work in groups of three to use Coulomb's Law \[\vec{E}(\vec{r}) =\frac{1}{4\pi\epsilon_0}\int\frac{\rho(\vec{r}^{\,\prime})\left(\vec{r}-\vec{r}^{\,\prime}\right)}{\vert \vec{r}-\vec{r}^{\,\prime}\vert^3} \, d\tau^{\prime}\] to find an integral expression for the electric field, \(\vec{E}(\vec{r})\), everywhere in space, due to a ring of charge.
In an optional extension, students find a series expansion for \(\vec{E}(\vec{r})\) either on the axis or in the plane of the ring, for either small or large values of the relevant geometric variable. Add an extra half hour or more to the time estimate for the optional extension.
assignment Homework
Instructions for 2022: You will need to complete this assignment in a 15 minute appointment on Zoom or in person with one of the members of the teaching team between 1/21 and 10 pm on 1/26. Here is a link to a sign-up page.
You are required to watch a sample video for how to make symmetry arguments here. As demonstrated in the video you should bring with you to the meeting a cylinder, an observer, and a vector.
Use good symmetry arguments to find the possible direction for the electric field due to a charged wire. Also, use good symmetry arguments to find the possible functional dependence of the electric field due to a charged wire. Rather than writing this up to turn in, you should find a member of the teaching team and make the arguments to them verbally.
group Small Group Activity
30 min.
group Small Group Activity
30 min.
assignment Homework
assignment Homework
assignment Homework
Which of the following forces can be central forces? which cannot? If the force CAN be a central force, explain the circumstances that would allow it to be a central force.