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LESSON 11 / 20 · TOPIC 8.4

A ring cancels transverse fields but keeps an axial field

You will be able to: Derive the axial electric field of a uniformly charged thin ring.

Calculus-based electrostaticsFree study resourceReview editionTeacher review pending

Why is a charged ring’s field zero at its center but nonzero along its axis?

At the center of a uniformly charged hoop, contributions from opposite sides cancel. Move along the line through its center perpendicular to its plane: the sideways contributions still cancel, but the axial parts now add.

A useful starting point: Symmetry cancels sideways contributions →

Words and symbols before equations

Ring radius R
Distance from the ring center to each source element.
Axis coordinate z
Signed distance from the ring center along its perpendicular axis.
Transverse
Perpendicular to the chosen axis.
Total charge Q
The sum ∫dq around the entire ring.
Ring axial field changes sign through the centerE_z (N/C)axis position z (m)-3-9.005-1.5-4.502001.54.50239.005
Read this model snapshot. Q = 2 nC, R = 1 m, z = 1 m: E_z = 6.364 N/C. For nonzero Q the magnitude peaks at |z| = 0.7071 m.
What this picture assumes

Uniform thin ring in the xy plane, center at origin, observation point on z axis. The optional projected 3D view illustrates geometry; rotating the camera leaves the same physical configuration and field. Diagram geometry is scaled, arrow length is directional only.

Read the picture in three steps

  1. Locate the labeled sources, system boundary or graph axes. Read the units before comparing values.
  2. Q = 2 nC, R = 1 m, z = 1 m: E_z = 6.364 N/C. For nonzero Q the magnitude peaks at |z| = 0.7071 m.
  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

At an axial point z, every ring element is at distance √(R² + z²). Its axial projection factor is z/√(R² + z²), including its sign. Thus dE_z = kz dq/(R² + z²)³ᐟ².

The distance and projection factor are the same for every element, so pull them outside ∫dq. This gives E_z = kQz/(R² + z²)³ᐟ². Uniform charge ensures transverse cancellation.

At z = 0 the field is zero even though charge is present all around. Far away, |E| approaches k|Q|/z². For positive Q and z > 0, the maximum occurs at z = R/√2, found by setting dE_z/dz = 0.

A worked example, step by step

A ring with R = 1 m carries Q = +2 nC. Find E at z = 1 m.

  1. Symmetry cancels all transverse components.
  2. Use E_z = kQz/(R² + z²)³ᐟ².
  3. E_z = 18/(2√2) = 6.36 N/C.
  4. The field points +z. At z = −1 m it has the same magnitude and opposite direction.
Common mix-up

The distance from an element is √(R² + z²), not z. The point-charge formula fails near the ring.

CHECK THE IDEA

Does zero E at the ring center mean there is no surrounding charge?

Compare with an explanation

No. Equal vector contributions cancel there.

Now investigate one change Explore →

Predict. Change one thing. Explain.

Slide the observation point through the center and find the maximum. Rotate the optional 3D projection to see the ring plane and axis; camera angle does not change E.

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

Ring axial field changes sign through the centerE_z (N/C)axis position z (m)-3-9.005-1.5-4.502001.54.50239.005

Q = 2 nC, R = 1 m, z = 1 m: E_z = 6.364 N/C. For nonzero Q the magnitude peaks at |z| = 0.7071 m.

Optional 3D view: ring plane and axisOptional 3D projection: ring and axis+z axisprobe z=1 mOrange ring in xy plane; purple probe lies on its perpendicular axis.

Use the view-angle control to rotate the projection. The field calculation stays fixed.

Uniform thin ring in the xy plane, center at origin, observation point on z axis. The optional projected 3D view illustrates geometry; rotating the camera leaves the same physical configuration and field. Diagram geometry is scaled, arrow length is directional only.

Explain what you noticed: Which quantity changed? Which stayed fixed? Use the relevant charge, vector superposition, electric field, flux or symmetry 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 center of a uniformly charged ring, E is…

Show answer and reasoning

zero. Opposite source contributions cancel.

2. For a positive ring, E_z at negative z is…

Show answer and reasoning

negative. The axial field points away from the ring plane on that side.

Original written challenge

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

For Q = +1 nC and R = 2 m, find E at z = 0 and z = 2 m, then state the far-field form.

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

Compare with the answer and four-point rubric
  1. 1 point: E(0) = 0 by symmetry.
  2. 1 point: At z = 2 m, E_z = 9(2)/(4 + 4)³ᐟ².
  3. 1 point: E_z = 0.796 N/C along +z.
  4. 1 point: For |z| much larger than R, |E| ≈ k|Q|/z².

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 1Which components cancel?

Components perpendicular to the ring axis.

RECALL 2What integral remains after symmetry?

∫dq = Q.

RECALL 3Does changing the camera change E?

No. It changes only the view of the same geometry.

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

A ring cancels transverse fields but keeps an axial field

  • E_z = kQz/(R² + z²)³ᐟ².
  • E_z(0) = 0; E_z(−z) = −E_z(z).
  • For fixed positive Q, the positive-axis maximum is at z = R/√2.

Remember: The distance from an element is √(R² + z²), not z. The point-charge formula fails near the ring.

Conditions: Uniform thin ring in the xy plane, center at origin, observation point on z axis. The optional projected 3D view illustrates geometry; rotating the camera leaves the same physical configuration and field. Diagram geometry is scaled, arrow length is directional only.

Refresh Kid · AP Physics C: Electricity and Magnetism Unit 1 (official Unit 8) · Objectives 8.4.A · Review edition

Framework, scope and review status

Mapped to College Board CED, Topic 8.4, objectives 8.4.A. CED effective Fall 2024, current PDF ©2026; checked September 16, 2026. This is E&M Unit 1: Electric Charges, Fields, and Gauss’s Law, numbered Unit 8 in the official combined Physics C sequence. Topics 8.1–8.6 retain their official identifiers. Quantitative force examples use at most four point charges. Field integrals use the specified rods, ring, arc and infinite wire; Gauss-law field calculations use spherical, cylindrical or planar symmetry. Optional projected 3D views clarify area normals and geometry; camera rotation never changes the physics. Checked with the Fall 2026 clarifications. 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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