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Online Electricity & Magnetism Tutoring

Tutoring in electric and magnetic fields, potential, circuits and electromagnetic induction.

Start with a concept you would like explained or a question you do not yet know how to begin. A course outline or an attempted solution can help if you have one. We confirm the level, topics and availability before booking. Tutoring sessions are currently offered in English. In-person options in Montréal

Electromagnetism and optics at McGill

Choose your exact course for worked examples and one-to-one help with fields, circuits or optics.

Choose the quantity or constraint first

These lessons cover selected electric-field, capacitor and circuit questions. Use your current course outline to choose the topics you need.

Connect changing flux to induced-current direction

Choose the viewing direction before saying clockwise or counterclockwise. The full lesson connects diagrams, Lenz’s law and the slope of flux, with six questions, hints and targeted retries. The calculus extension is labelled separately; follow your section’s methods.

Explain Faraday’s sign and the current direction

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Topics covered

Electric force and fieldsElectric potential and energyGauss’ lawCapacitance and circuitsMagnetic fields and forcesElectromagnetic induction

Common difficulties

  • Distinguishing field, force, potential, and energy
  • Using symmetry and signs
  • Connecting circuits to physical relationships

How tutoring can help

Tell us which idea you’d like to understand, or bring a circuit, a field diagram or a question. We can start with the basic concepts. A tutor can help you identify what stays fixed, choose the relationship, check signs and units, then work through a similar problem with you. Share your topic and preferred times; we confirm the scope and availability before booking.

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A practice example

Field and force are not interchangeable

Let E\mathbf E denote a uniform electric field pointing right. A small test charge has signed charge q<0q<0. In which direction does the electric force F\mathbf F on that charge point?

Work through the reasoning

The relation is F=qE\mathbf F=q\mathbf E: multiply the field vector by the signed charge. Multiplication by a negative number reverses a vector’s direction, so the force points left. Its magnitude is ∣q∣ ∥E∥|q|\,\lVert\mathbf E\rVert, where ∣q∣|q| is the absolute value of the charge and ∥E∥\lVert\mathbf E\rVert is the field vector’s magnitude. The field describes the influence of the source charges at the observation point; the force also depends on the test charge placed there. A positive test charge would feel a force to the right in this same field. Draw those two cases before doing longer component calculations.

Prepare for your lesson

Bring a diagram that separates the source charges, the observation point and the test charge. Label the field direction before finding the force direction. Keep the charge’s sign when multiplying a field vector, and use the absolute value only when calculating a magnitude.

An original Nablio example, not a university exam question. Your current course outline determines the material to focus on.

The connection chooses what stays fixed

An ideal 2 µF capacitor with no leakage is charged to 6 V. Its capacitance is then changed to 4 µF. Compare two separate cases: it stays connected to an ideal 6 V source, or it is disconnected first and remains isolated. Which quantity stays fixed, and what are the final charge and stored energy?

Follow the reasoning

Let C be capacitance, V the potential difference (voltage), Q the stored charge and U the stored energy. The prefix µ means one millionth: µF is microfarads, µC is microcoulombs and µJ is microjoules.

Start with the initial state: Q = CV = (2 µF)(6 V) = 12 µC. The energy is U = ½CV² = ½(2 µF)(6 V)² = 36 µJ. In these units, µF × V gives µC, and µF × V² gives µJ.

Connected: the ideal source holds V at 6 V. With C = 4 µF, Q = CV = 24 µC and U = ½CV² = 72 µJ.

Isolated: charge cannot enter or leave, so Q stays at 12 µC. With C = 4 µF, V = Q/C = 3 V and U = Q²/(2C) = 18 µJ.

The same capacitance change gives different results because the constraints differ. The stored energy changes: the source and/or the mechanism changing the capacitance can exchange energy.

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Exam preparation

What to practise

Exam preparation can combine conceptual field questions with calculations involving potentials, circuits, magnetic forces, and induction.

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