| Lesson Plan |
| Grade: |
Date: 01/12/2025 |
| Subject: Physics |
| Lesson Topic: use V = Q / (4πε0r) for the electric potential in the field due to a point charge |
Learning Objective/s:
- Describe the relationship between electric field and electric potential for a point charge.
- Apply V = Q / (4π ε₀ r) to calculate electric potential given charge and distance.
- Analyse sign and unit conventions when using the formula.
- Solve typical A‑Level style problems involving point‑charge potentials.
- Identify common errors such as sign mistakes and incorrect unit conversion.
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Materials Needed:
- Projector or interactive whiteboard
- Slide deck with derivation and example
- Worksheet with practice questions
- Scientific calculators
- Ruler/measure tape for demonstration
- Whiteboard and markers
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Introduction:
Begin with a quick recall of the electric field concept and ask students to predict how the potential varies with distance from a charge. Highlight that today’s success criteria are to derive the potential formula, use it correctly, and spot common mistakes.
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Lesson Structure:
- Do‑now (5') – Students answer a short slip‑sheet question on the link between E and V.
- Mini‑lecture (10') – Derive V = Q/(4π ε₀ r) from the line‑integral of the field, emphasising sign and units.
- Guided example (10') – Work through the +5 µC, r = 0.20 m problem; students fill steps on the worksheet.
- Interactive practice (15') – Pairs solve three practice questions while the teacher checks for the listed pitfalls.
- Concept check (5') – Quick poll/exit ticket: write the correct expression for potential and one common error to avoid.
- Summary (5') – Recap the inverse‑distance law and its importance for upcoming topics on equipotential surfaces.
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Conclusion:
Summarise that the potential of a point charge follows an inverse‑distance relationship and that careful handling of sign and units is essential. For the exit ticket, students calculate the potential 0.10 m from a –2 µC charge. Homework: complete the additional worksheet problems and read the next section on electric potential energy.
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