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Atlas MCAT Course

Equations & How to Use Them → Equations: Charge

Equations: Charge

Fields, circuits, capacitors, and electrochemistry.

01The idea

Charges move, fields exist, or energy is transferred electrically. Electrons move; cells generate voltage; ion gradients create potentials.

THREAD · Gradients and flow

02Build the model

AElectric charge: the property that creates electrical interaction

q = ne

Use when: counting charge; comparing magnitudes of charge; discrete charges are involved.

Passage cues: “Elementary charge”, “Number of electrons”, “Ionization”.

Don’t use it for: continuous charge distributions; field or force questions directly.

BCoulomb’s law: how charges exert forces on each other

F = kq₁q₂ / r²

Use when: two (or more) point charges interact; you care about force magnitude or direction; distance changes matter.

Passage cues: “Attraction / repulsion”, “Separated by distance r”, “Point charges”.

Don’t use it for: continuous charge distributions; circuit problems.

CElectric field: force per unit charge

E = F / q = kq / r²

Use when: a charge experiences force due to surroundings; you want a location-based description; test charge language appears.

Passage cues: “Field strength”, “Test charge”, “Region of space”.

Don’t use it for: energy-per-charge questions (use electric potential).

DElectric potential (voltage): energy per unit charge

V = U / q
ΔU = qΔV

Use when: energy changes are discussed; charges move due to potential difference; batteries or membranes appear.

Passage cues: “Potential difference”, “Energy gained/lost”, “Voltage source”.

Don’t use it for: force-based questions; pure current calculations.

EElectric field and voltage: how voltage creates force

E = V / d

Use when: uniform fields; parallel plates; distance between electrodes matters.

Passage cues: “Uniform field”, “Parallel plates”, “Separated by distance d”.

Don’t use it for: non-uniform fields; point charges.

FOhm’s law: what sets current

V = IR

Use when: steady-state circuits; comparing current, resistance, or voltage; resistors are present.

Passage cues: “Battery”, “Resistor”, “Steady current”.

Don’t use it for: capacitors charging/discharging; non-ohmic materials.

GElectric power: how fast electrical energy is transferred

P = IV = I²R = V²/R

Use when: energy per time matters; heat dissipation; comparing device output.

Passage cues: “Power”, “Energy per second”, “Heat generated”.

Don’t use it for: static fields; pure charge calculations.

HCapacitance and capacitor energy: ability to store charge and energy

C = Q / V
U = ½CV²

Use when: charge storage is discussed; capacitors appear; voltage changes without current flow; energy storage is asked.

Passage cues: “Capacitor”, “Dielectric”, “Stored charge”, “Charged capacitor”.

Don’t use it for: steady current flow; resistor-only circuits.

IRC time constant: how fast capacitors charge and discharge

τ = RC

Use when: charging/discharging curves; time-dependent behavior; exponential changes.

Passage cues: “Time constant”, “Exponential”, “Approaches equilibrium”.

Don’t use it for: pure DC steady-state; no capacitor present.

JSeries and parallel circuits: how components share current and voltage

Series: R_eq = R₁ + R₂ + …
Parallel: 1/R_eq = 1/R₁ + 1/R₂ + …

Use when: multiple resistors present; circuit architecture matters.

Passage cues: “Same current” (series), “Same voltage” (parallel).

KCell potential and free energy: electrical work available from redox

ΔG = −nFE

Use when: galvanic/voltaic cell spontaneity; relating voltage to free energy.

LNernst equation: how concentration gradients change voltage

E = E° − (RT / nF) ln Q

Use when: non-standard conditions (cell, physiology, electrochem); ion gradients / membrane potentials.

Passage cues: “Not standard conditions”, “Ion gradient”, “Membrane potential / equilibrium potential”.

03See the connections

The lesson names these links itself. Read the map left to right.

Electrostatics

  • Coulomb, field, potential
  • E = V/d

Circuits

  • V = IR, P = IV
  • Series vs parallel
  • C, U = ½CV², τ = RC

Electrochemistry

  • ΔG = −nFE
  • Nernst

Next: reactions.

04Reason with it

Four questions. Answer in your head first, then choose. You’ll see the reasoning either way.

Think first.

A question asks how much energy an ion gains crossing a membrane with a known voltage. Which relationship?

Think first.

A capacitor is charging through a resistor. Why is V = IR across the whole circuit not enough to describe it?

Think first.

A membrane’s ion gradient doubles in size. Which equation predicts a larger equilibrium potential?

Think first.

Two charges move three times farther apart. What happens to the force between them?

05MCAT lens

MCAT shortcuts

Closer charges → dramatically stronger force

Voltage = energy carried per charge

Voltage pushes, resistance resists

Series splits voltage, parallel splits current

Big R or C → slow response

Bigger gradient → bigger driving voltage

06Common traps

Trap 1: Treating voltage like force

Misconception

Voltage is energy per charge, not a push itself.

Correct model

Fields give forces; voltage gives energy.

Trap 2: Using Ohm’s law during capacitor charging

Misconception

Ohm’s law only applies after equilibrium.

Correct model

Use the RC time constant for time-dependent behavior.

Trap 3: Forgetting inverse-square behavior

Misconception

Distance matters a lot for fields and forces.

Correct model

F and E ∝ 1/r².

07Dependency check

Can you reconstruct this concept without looking at the page? You should now be able to reason through:

When to use field vs voltage

Check against 02 · C and D.

How circuits share current and voltage

Check against 02 · F and J.

How capacitors behave over time

Check against 02 · H and I.

How voltage links to free energy and gradients

Check against 02 · K and L.

If something feels unclear, the missing idea is usually thisForce questions use fields; energy questions use voltage; flow questions use circuits.

08Remember

REMEMBER · if you keep only a few things

  • F = kq₁q₂/r²; E = kq/r².
  • V = U/q; ΔU = qΔV; E = V/d.
  • V = IR; P = IV.
  • C = Q/V; U = ½CV²; τ = RC.
  • Series: resistances add. Parallel: reciprocals add.
  • ΔG = −nFE; Nernst: gradient → voltage.

09Forward hook

Electrochemistry ties voltage to free energy. The next block asks whether, and how fast, reactions go.

Which equation applies to spontaneity, equilibrium, and reaction rates?

That leads to the reaction equations.

Next lesson
Equations: Reactions
→