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LESSON 08 / 18 · TOPIC 10.3

Read and combine electric field vectors

You will be able to: Use field-map directions and superposition without adding magnitudes blindly.

Official College Board Unit 10Free study resourceReview editionTeacher review pending

Where do fields cancel and where do they reinforce?

At the midpoint between two equal positive charges, one field points right and the other left, so the net field is zero. Change the right charge to negative: both midpoint fields point right and reinforce.

A useful starting point: A field describes a place; force acts on a charge →

Words and symbols before equations

Observation point
The position where the field is evaluated; exclude a point source’s own location.
Vector map
Arrows showing local field directions and strengths.
Field line
A curve tangent to the field direction; closer lines represent stronger field in a consistent diagram.
Superposition
Add the vector fields from each source, component by component.
Point-charge field slice · direction-only arrowsProbe at x=0; axes in meters. Source neighborhoods omitted.+1 nC+1 nCprobe y=0 mx: −1 mx: +1 m
Read this model snapshot. At (0,0) m: E_x=0 N/C, E_y=0 N/C, |E|=0 N/C. Field vectors cancel at this probe. Map arrow length is normalized, not a strength scale.
What this picture assumes

Sources +1 nC at (−0.5,0) m and ±1 nC at (+0.5,0) m. Map arrows are normalized to a common length and show direction only, not strength. Quantitative components are given at (0,y); source neighborhoods are omitted. Map is a 2D slice of a 3D point-charge field.

Read the picture in three steps

  1. Locate the labeled sources, system boundary or graph axes. Read the units before comparing values.
  2. At (0,0) m: E_x=0 N/C, E_y=0 N/C, |E|=0 N/C. Field vectors cancel at this probe. Map arrow length is normalized, not a strength scale.
  3. Check what the picture assumes below. Use the Explore task to predict one change before moving a control.

Connect the picture to the physics

For each source draw the field at the observation point away from positive charge or toward negative charge. Then add components. Signs of charges determine directions, not a scalar subtraction shortcut that works everywhere.

At a point above the center of two equal positive charges, horizontal components cancel and vertical components add. This is a different result from the midpoint on the line. Symmetry is useful only after identifying which components it relates.

Field lines do not cross where the field has a unique nonzero direction. The explorer uses normalized arrows for direction only, with a separate quantitative readout at a probe. Arrow length therefore does not encode field strength in this particular map.

A worked example, step by step

Equal charges +1 μC sit at x=−0.5 m and +0.5 m. Find E at x=0. Then reverse the right charge.

  1. Each source is 0.5 m from the midpoint.
  2. Each field magnitude is 9×10⁹(10⁻⁶)/(0.5)²=36000 N/C.
  3. Two positive charges give equal opposite midpoint fields: E_net=0.
  4. With the right charge negative, both fields point right: E_net=72000 N/C.
Common mix-up

A zero field at one point does not mean there are no source charges or that potential is zero there.

CHECK THE IDEA

Can equal opposite charges have zero midpoint field?

Compare with an explanation

No. Their midpoint fields point from positive toward negative and add.

Now investigate one change Explore →

Predict. Change one thing. Explain.

Switch between equal like charges and an opposite-charge pair. Move the probe vertically along the midpoint line. Predict which components cancel before reading E_x and E_y.

On narrow screens, swipe or scroll diagrams sideways to read all labels.

Point-charge field slice · direction-only arrowsProbe at x=0; axes in meters. Source neighborhoods omitted.+1 nC+1 nCprobe y=0 mx: −1 mx: +1 m

At (0,0) m: E_x=0 N/C, E_y=0 N/C, |E|=0 N/C. Field vectors cancel at this probe. Map arrow length is normalized, not a strength scale.

Sources +1 nC at (−0.5,0) m and ±1 nC at (+0.5,0) m. Map arrows are normalized to a common length and show direction only, not strength. Quantitative components are given at (0,y); source neighborhoods are omitted. Map is a 2D slice of a 3D point-charge field.

Explain what you noticed: Which quantity changed? Which stayed fixed? Use the relevant charge, field or energy relationship to justify your prediction.

Apply the idea to a fresh problem Practice →

Show what you understand.

Two original questions are a starting check, not proof of mastery. Explain your choice before revealing the answer.

1. At the midpoint of two equal positive charges, net E is…

Show answer and reasoning

Zero. Equal opposite source fields cancel at that point.

2. Field lines cannot cross at a point with nonzero E because…

Show answer and reasoning

The field has one vector direction there. A crossing would assign two different tangent directions to one vector.

Original written challenge

4 points · self-check · not an official AP question

Two equal positive charges lie left and right of the origin. A probe is directly above the origin. (a) Draw each source field. (b) Compare x-components. (c) Compare y-components. (d) State net direction.

This response is not submitted or saved. Copy it before leaving.

Compare with the answer and four-point rubric
  1. 1 point: Both point away from their sources toward the elevated probe.
  2. 1 point: Equal magnitudes with opposite signs cancel.
  3. 1 point: Both upward and equal, so they add.
  4. 1 point: Net field upward.

Accept equivalent correct methods and explanations. This is a Refresh Kid teaching rubric, not an official AP scoring guideline.

Recall the ideas without notes Review →

Retrieve it before you reveal it.

RECALL 1What do field lines indicate?

Tangent direction and, with consistent line density, relative strength.

RECALL 2What is superposed?

Field vectors at the same observation point.

RECALL 3Does E=0 force V=0?

No. Vector field and scalar potential can cancel differently.

Revisit these tomorrow and a week later. Try a fresh problem and explain why the method applies.

Read and combine electric field vectors

  • E_net=ΣE_i as vectors.
  • Point source magnitude: k|Q|/r².
  • Direction-only arrows must not be used to infer magnitude.

Remember: A zero field at one point does not mean there are no source charges or that potential is zero there.

Conditions: Sources +1 nC at (−0.5,0) m and ±1 nC at (+0.5,0) m. Map arrows are normalized to a common length and show direction only, not strength. Quantitative components are given at (0,y); source neighborhoods are omitted. Map is a 2D slice of a 3D point-charge field.

Refresh Kid · AP Physics 2 Unit 2 (official Unit 10) · Objectives 10.3.A · Review edition

Framework, scope and review status

Mapped to College Board CED, Topic 10.3, objectives 10.3.A. CED effective Fall 2024, current PDF ©2026; checked September 16, 2026. Refresh Kid calls this the second AP Physics 2 unit; College Board numbers it Unit 10; the first unit in this course is official Unit 9. The lesson breakdown and questions are original Refresh Kid work, not official topic subdivisions.

Implementation and automated checks are separate from independent teacher review and observation of students. Both human review stages remain pending. This is a review edition, not a certified or validated assessment.

Optional further resource: College Board’s released questions and scoring guides. Papers can combine units; this link is an archive, not an assignment of every question to this lesson.

Our learn, explore, practice and recall sequence is informed by the IES learning guide. The exact Refresh Kid implementation has not been evaluated for learning effectiveness.

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