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Circuits Part 2: EMF & Capacitors

EMF and internal resistance, meters, capacitors and dielectrics, RC circuits, and bioelectricity

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Circuits Part 2: EMF & Capacitors

EMF and Real Batteries

A real battery is an ideal EMF in series with an internal resistance: Vterminal=ฮตโˆ’IrV_{terminal} = \varepsilon - Ir, so terminal voltage sags as more current is drawn. Ammeters go in series with almost no resistance; voltmeters go in parallel with very high resistance.

Capacitors

C=QVC=ฮบฮต0AdU=12CV2C = \frac{Q}{V} \qquad C = \kappa\varepsilon_0\frac{A}{d} \qquad U = \tfrac{1}{2}CV^2 A dielectric raises capacitance. With the battery connected, voltage is fixed; disconnected, charge is fixed. Capacitors combine opposite to resistors: directly in parallel, reciprocally in series.

RC Circuits

An uncharged capacitor acts like a wire the instant a switch closes and like a break once charged. The time constant ฯ„=RC\tau = RC sets the pace: about 63% charged after one ฯ„\tau, essentially full after about 5ฯ„5\tau.

Bioelectricity

The cell membrane is a capacitor (the bilayer) in parallel with resistors (the ion channels). Myelin lowers membrane capacitance and raises membrane resistance, speeding conduction. A defibrillator stores energy in a capacitor and releases it in a brief pulse.

Key Takeaways

  • Terminal voltage is below the EMF whenever current flows out of a battery.
  • Decide first whether Q or V is held constant, then choose the energy formula.
  • Capacitor combination rules are the reverse of resistor rules.
  • Steady state: no current through a capacitor branch.
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๐Ÿ“Œ Related Topics in Chemical & Physical Foundations

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EMF and internal resistance, meters, capacitors and dielectrics, RC circuits, and bioelectricity
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