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United StatesPhysics C: Electricity and MagnetismSyllabus dot point

How does inserting a dielectric change a capacitor's capacitance, field, voltage and stored energy?

Topic 10.4 Dielectrics: explain how a dielectric increases capacitance and analyze the field, voltage and energy of a capacitor with a dielectric.

A calculus-based answer to AP Physics C E&M Topic 10.4, covering the dielectric constant, polarization, how a dielectric raises capacitance, and the changes to field, voltage and energy at fixed charge or fixed voltage.

Generated by Claude Opus 4.810 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this topic is asking
  2. Polarization and the dielectric constant
  3. Capacitance with a dielectric
  4. Fixed charge versus fixed voltage
  5. Try this

What this topic is asking

The College Board (Topic 10.4) wants you to explain how inserting a dielectric (an insulator) into a capacitor increases its capacitance, and to analyze the resulting changes in field, voltage and stored energy, carefully distinguishing the case of fixed charge (isolated capacitor) from fixed voltage (battery attached).

Polarization and the dielectric constant

When a dielectric fills a capacitor, the polarized molecules build up bound surface charge that sets up a field opposing the original. The net field inside is reduced to E=E0κE = \dfrac{E_0}{\kappa}, so for the same free charge the voltage V=EdV = Ed is smaller, and capacitance C=Q/VC = Q/V is larger.

Capacitance with a dielectric

Inserting a dielectric multiplies the capacitance by κ\kappa:

C=κC0=κε0AdC = \kappa C_0 = \frac{\kappa\varepsilon_0 A}{d}

The quantity κε0\kappa\varepsilon_0 is sometimes written ε\varepsilon, the permittivity of the material. Practically, dielectrics let capacitors be physically small yet hold a large capacitance, and they raise the voltage the capacitor can tolerate before the insulator breaks down and conducts.

Fixed charge versus fixed voltage

The key exam skill is tracking what stays constant when the dielectric goes in:

Held fixed QQ CC V=Q/CV = Q/C EE UU
Charge (isolated) same ×κ\times\kappa ÷κ\div\kappa ÷κ\div\kappa ÷κ\div\kappa
Voltage (battery on) ×κ\times\kappa ×κ\times\kappa same same ×κ\times\kappa

Try this

Q1. A 2.0μF2.0\,\mu\text{F} capacitor has a dielectric of κ=5\kappa = 5 inserted. Find the new capacitance. [1 point]

  • Cue. C=κC0=(5)(2.0)=10μFC = \kappa C_0 = (5)(2.0) = 10\,\mu\text{F}.

Q2. State what happens to the field inside a capacitor when a dielectric of constant κ\kappa is inserted at fixed charge. [1 point]

  • Cue. The field falls to E0/κE_0/\kappa (the polarized dielectric partly cancels it).

Exam-style practice questions

Practice questions written in the style of College Board exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

AP 2021 (style)1 marksSection I (multiple choice). An isolated (disconnected) charged parallel-plate capacitor has a dielectric of constant κ=3\kappa = 3 inserted to fill the gap. The potential difference across it (A) triples (B) is unchanged (C) falls to one third (D) falls to one ninth. Justify your reasoning.
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A 1-point MCQ on a dielectric at fixed charge. The answer is (C).

Isolated means QQ is fixed. Capacitance rises to κC\kappa C. Since V=Q/CV = Q/C, with QQ fixed and CC tripled, VV falls to one third. The trap is (A): voltage rises only if you instead held VV... but here QQ is fixed, so VV drops.

AP 2024 (style)5 marksSection II (FRQ, quantitative). A parallel-plate capacitor with C0=4.0μFC_0 = 4.0\,\mu\text{F} is charged by a 5050 V battery and then **disconnected**. A dielectric with κ=2.5\kappa = 2.5 is then inserted. (a) State whether the charge changes and why. (b) Calculate the new voltage. (c) Calculate the change in stored energy and explain where the energy went.
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A 5-point FRQ on a dielectric inserted at fixed charge.

(a) Charge (1 point): disconnected, so QQ is fixed: Q=C0V0=(4.0×106)(50)=2.0×104Q = C_0 V_0 = (4.0\times10^{-6})(50) = 2.0\times10^{-4} C.
(b) New voltage (2 points): new capacitance C=κC0=10μFC = \kappa C_0 = 10\,\mu\text{F}. V=QC=2.0×10410×106=20V = \dfrac{Q}{C} = \dfrac{2.0\times10^{-4}}{10\times10^{-6}} = 20 V.
(c) Energy (2 points): U0=Q22C0=(2.0×104)22(4.0×106)=5.0×103U_0 = \dfrac{Q^2}{2C_0} = \dfrac{(2.0\times10^{-4})^2}{2(4.0\times10^{-6})} = 5.0\times10^{-3} J; U=Q22C=2.0×103U = \dfrac{Q^2}{2C} = 2.0\times10^{-3} J. The energy falls by 3.0×1033.0\times10^{-3} J; the dielectric is pulled in, so the field does work on it (and energy dissipates), lowering the stored energy.

Markers reward fixed QQ, the new VV, and the energy decrease with a physical reason.

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