PART 0 Primer
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Electrical Theory Foundations

Read first if EE is new to you

Power Atlas assumes you know the fundamentals — what voltage is, why we use AC, what reactive power means physically. This page covers all of it. After reading, §01's formulas will make sense, not just be memorized.

First-read path — if this is your first day with EE
This page is dense (48 sub-sections). On a first pass, read these essentials in order, then come back for the rest after §11/§12:
  1. The Three Quantities + Ohm's Law — voltage, current, resistance, the foundational equation.
  2. Kirchhoff's Laws (KVL + KCL) — how voltage adds around loops; how current splits at nodes.
  3. DC vs AC + The Sinusoid — why we use AC; what RMS means.
  4. Why Three-Phase Is the Standard + The Magic of Transformers — the two ideas that built the grid.
  5. The Hill Metaphor + Power Triangle = Beer Glass — pictures for voltage/current/energy and real/reactive/apparent power.

Skip on first read: Phasors, Symmetrical Components, Per-Unit. Return to these when §11/§12 (short-circuit + per-unit math) make you want them.

The Three Quantities — Voltage, Current, Resistance

QuantitySymbolUnitPlumbing analogyElevator analogyWhat it physically is
VoltageVVolt (V)Water pressure between inlet and outlet (PSI)Floor-to-floor height difference — the up/down journey the elevator deliversElectrical potential difference between two points — the "push" that wants to move charge.
CurrentIAmpere (A)Water flow rate through a pipe (gal/min)People riding — when multiple elevators serve the same floors, the crowd splits among themCharge flowing per second (coulombs per second). Read with a clamp meter on a single conductor.
ResistanceROhm (Ω)Pipe friction — narrower or longer pipe opposes flow moreSlow elevator, long door dwell, queue at the lobby — what limits how many can ride per minuteOpposition to current flow. Depends on conductor size, length, and material.
PowerPWatt (W)Water power: pressure × flow (PSI × GPM)People × floors per minute being movedRate of energy transfer. P = V × I.
EnergyEWatt-hour (Wh)Total water moved over timeTotal people × floors moved over the dayPower × time. What the utility bills you for (kWh).

Ohm's Law — The Foundational Equation

Voltage equals current times resistance. Memorize the triangle: cover what you want to find, the formula appears.

Three forms of one equation
V = I × R
I = V / R
R = V / I
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Concrete example
A 12V car battery connected to a headlight bulb with R = 6 Ω draws I = 12/6 = 2 A. The bulb consumes P = V × I = 12 × 2 = 24 W. If the headlight runs 1 hour, energy used = 24 Wh = 0.024 kWh.

Kirchhoff's Laws — How Current and Voltage Behave in Circuits

LawStatementWhat it means in practice
KVL — Kirchhoff's Voltage LawSum of voltages around any closed loop = 0Voltage drops across components in a loop add up to the source voltage. Why we calculate voltage drop along a feeder + branch + load = source voltage.
KCL — Kirchhoff's Current LawSum of currents entering a node = sum of currents leavingCurrent splits at a junction in proportion to inverse impedance. Why parallel branches share current. Why neutral current is the unbalanced sum of phase currents.
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The elevator analogy for KCL
A bank of three elevators serves the same lobby. Voltage is the up/down journey — the floors any one of them can travel. Current is the crowd of people: when 60 riders show up at the lobby and there are three elevators, the crowd splits among them. The fastest elevator (lowest "impedance") gets the largest share; a slow one with sticky doors gets fewer riders. The crowd entering the lobby equals the sum of crowds leaving in the three cars — that's KCL. If one elevator is out of service (open circuit), its share redistributes to the others. If two elevators are identical in speed, they split the crowd 50/50.
KVL — Voltage Loop Sum of voltages around any loop = 0 + Vs = 12V R₁ V₁ = 8V R₂ V₂ = 4V loop Vs − V₁ − V₂ = 0 12 − 8 − 4 = 0 ✓
Battery raises voltage; resistors drop it. Around any closed loop, the rises and drops cancel.
KCL — Current Node Σ currents in = Σ currents out at any node node I₁ = 5A in I₂ = 3A in I₃ = 6A out I₄ = 2A out 5 + 3 = 6 + 2 ✓
Charge can't accumulate at a node. What flows in must flow out — total in = total out.

DC vs AC — Why We Use Alternating Current

DC (Direct Current)AC (Alternating Current)
Direction of flowOne direction, constantReverses 60 times per second (US) or 50 (Europe)
Voltage transformationHard — requires DC-DC converters (inefficient at scale)Easy — passive transformer steps up/down with ~ 99% efficiency
Long-distance transmissionLossy at low voltage; requires HVDC for long distance (specialized + expensive)Easy — step up to MV/HV, transmit, step down. I²R losses minimized.
Where usedBatteries, electronics, telecom, EV tractionEverything between the power plant and the wall outlet
Why it won (1880s)The transformer made AC scalable. Tesla + Westinghouse beat Edison's DC for distribution.

The Sinusoid — What "AC" Actually Looks Like

+Vpeak -Vpeak 0 time RMS = Vpeak / sqrt(2) = 0.707 x Vpeak Peak 1 cycle = 16.67 ms (60 Hz) A 120V outlet has Vpeak = 170V. RMS = 120V is what your meter reads.
RMS = the equivalent DC voltage that would produce the same heating in a resistor. Always use RMS for AC power calculations.

Frequency — Why 60 Hz?

60 Hz is the US/North America standard. 50 Hz is most of Europe + Asia. Higher frequency = smaller transformer cores (good) but more transmission line losses (bad). 60 Hz was Westinghouse's choice; 50 Hz was AEG's. Both work; the world settled on regional standards by ~1920.

Why Three-Phase Is the Standard

Three sinusoids, equal magnitude, 120° apart. Why this beats single-phase and 2-phase:

PropertyWhy 3-phase wins
Constant total instantaneous powerP1(t) + P2(t) + P3(t) = constant. (For 1-phase, total power pulses at 120 Hz. For 2-phase, it pulses too.) Constant power = smooth motor torque, no vibration.
Minimum copper for transmission3 wires for the same kW vs 2 wires for 1-phase = ~ 25% LESS copper per kW transmitted. (4 wires for 2-phase = WORSE.) This is why utilities use 3-phase everywhere.
Self-starting motors3-phase produces a uniform rotating magnetic field. Motor starts on its own. (1-phase motors need start capacitors or shaded poles.)
Neutral can be omittedBalanced 3φ has zero current in the neutral — can use 3 wires only. (Unbalanced loads need a neutral.)

The Magic of Transformers — Why AC Won

Faraday's Law (1831) — a changing magnetic field induces voltage in a nearby conductor. AC's constant change makes this practical:

  1. AC current in primary winding creates a changing magnetic flux in the iron core.
  2. The changing flux induces a voltage in the secondary winding.
  3. The voltage ratio = the turns ratio: V₁/V₂ = N₁/N₂.
  4. Power is conserved (minus tiny losses): V₁ × I₁ = V₂ × I₂. Step up voltage → step down current.

Why this matters: at the power plant, generate at 13.8 kV. Step up to 230 kV for transmission (low current = low I²R losses). Step down to 12.47 kV for distribution. Step down to 480V at the building. Step down to 120V at the outlet. Five voltage levels, five transformers, one path.

PRIMARY N₁ turns V₁, I₁ SECONDARY N₂ turns V₂, I₂ Φ flux V₁/V₂ = N₁/N₂
Iron core couples primary AC magnetic flux to secondary winding. Step up V → step down I.

Resistance + Inductance + Capacitance — The Three Passive Elements

ElementSymbolWhat it doesHow it acts in ACPhase relationship
ResistorRDissipates energy as heat. Pure friction.Voltage and current rise/fall together. No energy storage.V and I IN PHASE (PF = 1.0)
Inductor (L) — coil of wire, motor windings, transformer primaryLStores energy in magnetic field. Resists changes in current.Voltage LEADS current by 90°. Current lags.I lags V by 90° (PF = 0)
Capacitor (C) — two metal plates separated by insulatorCStores energy in electric field. Resists changes in voltage.Voltage LAGS current by 90°. Current leads.I leads V by 90° (PF = 0)

Why this matters: Reactive Power Explained Physically

An inductor (motor coil) doesn't dissipate energy — it stores energy in its magnetic field, then releases it. The current flowing back and forth creates this storage/release cycle. The current is real (you have to size wires for it), but no NET energy gets used.

This is what reactive power (Q, in kVAR) is — the apparent flow of power that just sloshes back and forth between source and load. It uses no fuel at the power plant but does use copper in the wires.

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Why utilities care about reactive power
A factory drawing 100 kW at PF = 0.8 actually has 100 kVA × current passing through utility transformers (because S = P/PF = 125 kVA). The utility sized infrastructure for 125 kVA but only collected revenue for 100 kW. Power factor correction (capacitors) cancels the inductive sloshing, brings PF closer to 1.0, and frees up utility capacity.

Impedance — Generalized Resistance for AC

For AC, the opposition to current isn't just resistance. It includes inductive reactance (XL) and capacitive reactance (XC) too.

Impedance (Z) magnitude
|Z| = √(R² + X²)
where X = XL − XC (net reactance). Z replaces R in Ohm's Law for AC: V = I × Z.
ReactanceFormulaNotes
Inductive (XL)XL = 2π × f × LHigher frequency → more reactance. (Why high-frequency harmonics get blocked by inductors.)
Capacitive (XC)XC = 1 / (2π × f × C)Higher frequency → LESS reactance. (Why capacitors short out high-frequency noise.)

Phasors — Why Engineers Draw Triangles

Each AC voltage or current is a sinusoid with magnitude AND phase angle. Adding two sinusoids of different phases is messy with trigonometry. Phasors represent each sinusoid as an arrow (length = magnitude, direction = phase angle), then you add the arrows like vectors.

Real (P) Reactive (Q) P (real) Q (reactive) S (apparent) theta Phasor Diagram = Power Triangle Same triangle as section 0 - rotated to show complex-plane interpretation
A phasor is just a 2D arrow in the complex plane. The power triangle (§01) is a phasor diagram.

Systematic Methods — Mesh and Nodal Analysis

KVL and KCL by themselves are great for two- or three-element circuits. Once a network gets bigger, you want a recipe — a systematic way to write equations and solve. Two methods, dual to each other.

MethodBuilt onUnknowns you solve forBest when…
Mesh (loop) analysisKVL — sum of voltages around each independent loop = 0Mesh (loop) currentsFew loops, lots of voltage sources
Nodal analysisKCL — sum of currents into each node = 0Node voltages relative to a chosen reference (ground)Few nodes, lots of current sources or parallel branches

Mesh recipe: (1) Label each independent loop with an assumed direction (clockwise convention). (2) For each loop, write KVL: assumed-direction source rises − sum of (loop current × resistance) drops − contributions from neighboring loops sharing a resistor = 0. (3) Solve the resulting linear system for the loop currents. Branch currents are then sums or differences of adjacent loop currents.

Nodal recipe: (1) Pick one node as reference (ground = 0 V). (2) Label every other node with an unknown voltage V1, V2, … (3) For each labeled node, write KCL — current leaving through each connected resistor = (Vthis node − Vother end) / R, summed to zero (with current sources added). (4) Solve the linear system for node voltages. Branch currents come from V/R afterward.

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Quick worked sweep — single mesh equation
A 24 V source drives two resistors in series: R1 = 4 Ω and R2 = 8 Ω. One loop, one mesh current I.
KVL: 24 − 4·I − 8·I = 0 → 12·I = 24 → I = 2 A. Each resistor's voltage drop comes from V = I·R. Same answer Ohm's Law gives directly — but the same recipe scales to 5, 10, 50 loops without re-deriving.

Why this matters in power systems: matrix-based mesh and nodal analysis is the foundation of power-flow software (Newton-Raphson on Y-bus admittance matrices is just nodal analysis at scale). It's also how relay coordination tools compute fault currents across an interconnected network — they reduce the system to a Thevenin equivalent at each candidate fault point, which is mesh/nodal applied recursively.

Series + Parallel Circuits

ConfigurationResistanceVoltageCurrent
Series (one path)Rtotal = R1 + R2 + ...V splits across each RSame I through every R
Parallel (multiple paths)1/Rtotal = 1/R1 + 1/R2 + ...Same V across every RI splits inversely to R
Two parallel resistors (special case)Rtotal = (R1 × R2) / (R1 + R2)
Plumbing analogyElevator analogy
Series — voltage One pipe with two restrictions in line. The total pressure drop from inlet to outlet equals the drop across the first restriction plus the drop across the second. Add them. One elevator shaft, two stops on the way down — lobby → mezzanine → basement. The total height drop is the sum of (lobby → mezzanine) and (mezzanine → basement). Voltage drops add along the path.
Series — current The same water flow rate moves through both restrictions in line. Whatever leaves the first restriction enters the second. One flow rate everywhere. The same crowd of people rides the single elevator past every floor. Twenty riders boarding the lobby = twenty riders passing mezzanine = twenty arriving at basement. One crowd, one count, every stop.
Parallel — voltage Two pipes splitting from the same manifold and rejoining at the same outlet. Both pipes see the same inlet-to-outlet pressure difference. Pressure is the same across both. Three elevators side by side, each running between the same two floors — lobby and the 30th floor. Every elevator delivers the same vertical journey. Voltage is the same across every parallel branch.
Parallel — current The total water flow into the manifold splits between the two pipes, with the smaller-restriction pipe carrying more flow. Inverse to resistance. Sixty people walk into the lobby; the three elevators split the crowd. The fastest elevator (lowest "impedance") gets the largest share; the sluggish one with sticky doors gets fewer. Current splits inversely to resistance.

Why this matters in power systems: branch circuits in a panel are in PARALLEL with each other (all share the bus voltage; current splits per load). Conductors in PARALLEL feeders share current proportionally to inverse impedance — equal-length matched conductors share equally; mismatched ones don't. NEC 310.10(H) requires identical termination + length for paralleled conductors precisely because of this. (When one of three "elevators" is slow, the other two overload — same physics as paralleled feeders with mismatched impedance.)

Superposition Principle

For any LINEAR circuit with multiple sources, the response (voltage or current) at any point equals the SUM of responses caused by each source individually (with all other sources turned off — voltage sources shorted, current sources opened).

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Where superposition applies in power systems
  • Multiple-source fault analysis: contribution from utility + on-site generation + motor back-feed. Sum each source's contribution to total fault current.
  • Power flow with co-generation: utility provides part of load, on-site PV provides rest. Solve each separately, sum.
  • Harmonic analysis: each harmonic frequency is solved separately, then summed (since circuit elements respond differently at each frequency).
Limitation: only works for LINEAR circuits. Doesn't apply to circuits with magnetic saturation (transformer cores at high flux) or semiconductor switches (VFD outputs).

Thevenin + Norton Equivalents

Any complex network of voltage sources, current sources, and resistors can be reduced to a single equivalent source with a single equivalent impedance, when viewed from any pair of terminals.

EquivalentWhat it isHow to find
Thevenin equivalent (Vth, Rth)Voltage source Vth in SERIES with resistance RthVth = open-circuit voltage at the terminals. Rth = resistance looking into the terminals with all sources zeroed.
Norton equivalent (In, Rn)Current source In in PARALLEL with resistance RnIn = short-circuit current at the terminals. Rn = Rth (same as Thevenin).
ConversionVth = In × Rn · In = Vth / Rth
Thevenin Equivalent Vth in SERIES with Rth ANY CIRCUIT (no matter how complex) replace with + Vth Rth A B Vth = open-circuit voltage at A–B Rth = R looking in with sources zeroed
Replace any complex circuit with one voltage source in series with one resistance.
Norton Equivalent In in PARALLEL with Rn ANY CIRCUIT (same as Thevenin) replace with A B In Rn In = short-circuit current at A–B Rn = Rth · In = Vth / Rth
Same circuit, current-source view. Norton and Thevenin are dual descriptions of the identical equivalent.
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Why Thevenin matters: it's how the utility looks to you
When the utility tells you "available fault current at the service is 50 kA at 12.47 kV," they're giving you a Thevenin equivalent of the entire grid behind your meter. Vth = 12.47 kV (no-load voltage), Rth = 12.47 kV / 50 kA = 0.144 Ω. The 50 kA is the Norton current (short-circuit current). Same information, two notations.

Symmetrical Components — Intro

Real power systems aren't perfectly balanced. Single-phase faults, ground faults, broken conductors all create UNBALANCED 3-phase conditions. Analyzing them with regular phasors is messy. Symmetrical components decompose any unbalanced 3-phase set into THREE balanced sets:

SequenceSymbolWhat it isWhen it exists
Positive sequenceV1, I1Balanced 3φ rotating ABCAlways present in normal operation
Negative sequenceV2, I2Balanced 3φ rotating ACB (reverse)Created by phase-phase faults, single-phasing of motors, unbalanced loads
Zero sequenceV0, I03 in-phase quantities (no rotation)Created by ground faults; flows in neutral; only exists in 4-wire systems

Each sequence has its own equivalent impedance for any piece of equipment. Faults are then analyzed by combining sequence networks. Full treatment in §12 Short Circuit.

Power = Energy / Time — kW vs kWh

The most common confusion in EE literacy. Let's nail it:

Power (kW)Energy (kWh)
What it isRate of energy transfer (instantaneous)Total energy moved over time
UnitWatt = Joule/sec; kW = 1000 WWatt-hour = 3600 J; kWh = 1000 Wh
Plumbing analogyFlow rate (gal/min)Total water moved (gallons)
MathkWh = kW × hours
What you're billed forDemand charge ($/kW)Energy charge ($/kWh)
Typical magnitudesHouse peak: 5-15 kW. Office: 50-500 kW. Atlas DC1: 5,000 kW.House annual: 10,000 kWh. Office annual: 1M kWh. Atlas DC1 annual: 44M kWh.

A 100W lightbulb running for 10 hours uses 1 kWh of energy at a power rate of 0.1 kW. Same lightbulb running for 1 hour: still 0.1 kW power, but only 0.1 kWh energy.

The Hill Metaphor — Voltage, Current, Energy

The plumbing analogy gets you started. The HILL metaphor goes deeper. It explains why voltage can exist without current, why batteries differ from capacitors, and why inductors and capacitors mirror each other.

Electrical conceptHill / gravity equivalent
Voltage (V)Height difference
Electric field (E)Gravity — the force pulling charges/balls
Current (I)Ball rolling / water flowing
Resistance (R)Friction along the path
Power (P)Rate energy is released as motion / heat / light
Energy (E)Total water moved · work done
Closed circuitA path the ball can roll DOWN and BACK UP (via the source)

Voltage Exists Without Current

A rock held 5 ft in the air
Height difference exists. Gravity exists. The rock is NOT moving. Potential energy is real but kinetic energy is zero.
🔋
A 9V battery on the table
Voltage exists. Electric field exists between terminals. Charges are NOT flowing. Connect a wire between terminals → the path closes → charges flow → current.

Voltage requires only an imbalance. Current requires a closed path. A battery without a circuit has voltage but zero current. The ball needs somewhere to roll TO before it falls.

Battery vs Capacitor — Chemistry vs Storage

BatteryCapacitor
MetaphorWorker repeatedly LIFTING the rock back to the top of the hillLifting the rock to the top ONCE
MechanismChemical reaction continuously moves charges from − to + terminalPump charges onto plates against the field; field stores them in place
"Dead" stateChemistry runs out — worker can't lift anymoreCharges flowed back through circuit — rock is back at the bottom
RechargeReverse the chemical reaction (charging the battery)Pump charges back onto plates (voltage source charges the cap)
Stored energyChemical bonds (the worker's stamina)Electric field between plates (the rock's height)
Voltage decayStays roughly constant until exhausted, then dropsDrops smoothly as charges flow off (V = Q/C)

The Electric Field — Where Is the Hill?

The electric field is created by charge separation. Move a positive charge somewhere it doesn't naturally want to be — separate it from a negative charge — and the resulting field is the "hill" between them.

  • Battery: chemistry creates and maintains the separation continuously.
  • Capacitor: external voltage forced charges apart; the cap holds them in place.
  • Open switch with charged cable: the cable is "lifted" by stored charge; voltage measured across the gap.
  • Static electricity: rubbing creates separation. Spark = the charges finally finding a path back across the gap.

Voltage isn't a "thing." It's the height difference. The field is the gravity. Charge separation is what builds the hill.

Inductor — The Flywheel

If a capacitor is "rock at height," an inductor is "spinning flywheel." They're not just different — they're opposite in every dimension.

DimensionCapacitorInductor
Stores energy inElectric field (between plates)Magnetic field (around coil)
Energy formulaE = ½CV²E = ½LI²
Stores variableVOLTAGE (V across plates)CURRENT (I through coil)
Resists changes inVoltage (V can't jump instantly — physics requires charge to accumulate)Current (I can't jump instantly — physics requires field to build)
Physical intuitionCompressing a spring (compressing charge separation)Spinning a flywheel (storing rotational energy)
What happens when source disconnectsHolds voltage (until leakage drains)Tries to maintain current — generates voltage spike (back-EMF)
"Open circuit" versionNo effect — already openCap-like: holds whatever charge the field had
"Short circuit" versionDischarges fast through wireNo effect — already short

The Flywheel Intuition for Inductors

Imagine a heavy flywheel on bearings:

ActionFlywheelInductor
Apply force / voltageSlowly accelerates — won't spin instantlyCurrent rises slowly — voltage causes I to ramp up over time
Stop pushingKeeps spinning by inertiaCurrent keeps flowing (briefly) by stored magnetic energy
Disconnect drive (open switch)Slows down via friction"Fights back" — current tries to flow, voltage spikes massively (V = -L · dI/dt)
Short the output (close path)Energy dissipates as heat in frictionStored energy released as heat in resistance
The flyback voltage spike — why every inductor circuit needs a path home
Open a switch in series with an inductor: the inductor desperately tries to maintain current. With no path, voltage rises until the air ITSELF breaks down — you see an arc across the switch contacts. This is why every solenoid, relay, contactor, and motor coil has a flyback diode across it: gives the current somewhere to circulate when the switch opens, and the back-EMF dissipates harmlessly. Forgetting the flyback diode kills your driver chip every time.

Charging + Discharging — Time Curves

Capacitor Charging DC voltage applied at t=0 through resistor 0 time → Vs t = τ V across cap (rising) V = Vs(1 − e−t/τ) I (decaying) I = (Vs/R)·e−t/τ τ = R·C — at t=τ cap is 63% charged
Cap starts empty: max current rushes in. As V builds, current drops. Steady state: V=Vs, I=0.
Inductor Charging DC voltage applied at t=0 through resistor 0 time → Vs t = τ I through coil (rising) I = (Vs/R)(1 − e−t/τ) V across L (decaying) V = Vs·e−t/τ τ = L/R — at t=τ current is 63% of max
Inductor starts at zero current: voltage holds the back-EMF. As I builds, V across L drops. Steady state: I=Vs/R, V=0.
Notice the symmetry — capacitor and inductor are MIRROR images
In a CAPACITOR, V rises slowly while I starts max + decays.
In an INDUCTOR, I rises slowly while V starts max + decays.
Swap V and I in the equations and the diagrams + you have the other component. This is what "duality" means in circuit theory.

Phase Relationships — Why Voltage Leads / Lags

For a Pure Capacitor: Current LEADS Voltage

Apply AC voltage to a cap. The cap can't have voltage without charge on its plates. Charges must arrive BEFORE the voltage builds up. So:

  1. Current flows TOWARD the cap (charging up).
  2. As charge accumulates, voltage rises BEHIND the current.
  3. When voltage peaks, current has already started to reverse (charge is starting to leave).
  4. Current LEADS voltage by 90° (a quarter cycle).

Memory aid: "ICE" — In a Capacitor, current (I) leads voltage (E).

For a Pure Inductor: Voltage LEADS Current

Apply AC voltage to an inductor. The inductor "fights" the rising current with a back-EMF. Current can't rise until voltage has been pushing for a while:

  1. Voltage rises across the coil.
  2. Current builds slowly behind it.
  3. When current peaks, voltage has already started decreasing.
  4. Voltage LEADS current by 90°.

Memory aid: "ELI" — in an inductor (L), voltage (E) leads current (I). Together: "ELI the ICE man" covers both.

ICE — Capacitor In a Capacitor: I leads V by 90° V (voltage) I (current) 90° "ICE" — In Capacitor, I-comes-before-E (voltage)
Capacitor needs charge BEFORE voltage builds. Current arrives first, then voltage rises.
ELI — Inductor In an inductor (L): V (E) leads I by 90° V (voltage / E) I (current) 90° "ELI" — Voltage (E) before I in inductor (L)
Inductor fights rising current with back-EMF. Voltage appears first; current builds behind.
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"ELI the ICE man" — the only mnemonic you need
In an L (inductor), E (voltage) comes before I (current) → ELI
In a C (capacitor), I comes before E → ICE
Combined: "ELI the ICE man" gives you both. The middle letter is the component; the first letter is what comes first in time.

Why Capacitors Are Used in Real Circuits

ApplicationWhat the cap doesWhere you see it
Filter cap (DC supplies)Smooths ripple after rectifier — caps charge during peaks, release during dipsEvery wall-wart, every PSU. Big electrolytic on the rail.
Coupling capBlocks DC offset, passes AC fluctuationAudio amplifiers, sensor signal chains
Decoupling / bypass capLocal current reservoir for fast IC switching — keeps voltage stable when chip suddenly draws currentEvery digital IC has 100 nF caps next to it
Power factor correctionCap supplies reactive current locally — cancels inductive lag from motorsIndustrial PFC banks (§14, §15)
Tuned circuit (with inductor)L and C resonate at specific frequency — extracts that frequency from a signalRadio receivers, harmonic filters, RF impedance matching
Energy storage (pulsed apps)Stores energy slowly, releases burst quicklyCamera flash, defibrillator, Tesla coils, UPS DC bus, particle accelerators
Snubber circuitAbsorbs voltage spikes during inductive switchingAcross relay contacts, in motor drives
Timing circuit (with R)RC time constant τ = R·C controls how fast V changes555 timers, retriggerable monostables, debouncers
Motor starting (split-phase)Cap creates a phase-shifted second winding — gives 1φ motor a starting torqueSingle-phase induction motors (HVAC compressors, well pumps)

Why Inductors Are Used in Real Circuits

ApplicationWhat the inductor doesWhere you see it
Filter inductor (choke)Smooths CURRENT ripple — opposite of cap which smooths voltageAudio amp output, switching power supply output, VFD output reactor
Current-limiting reactorSeries inductance limits inrush currentSoft-start motor drives, MV switchgear sub-transient current limiting
Transformer windingCreates the magnetic flux that couples primary to secondaryEvery transformer (§09)
Motor / generator windingCreates the rotating field that produces torque (or extracts torque)Every electric motor + generator
Tuned circuit (with cap)L and C resonate at specific frequencyRadio receivers, harmonic filters
EMI filterInductor blocks high frequency, passes low (impedance Z = 2πfL grows with f)Common-mode chokes on power cords, ferrites on cables
Energy storage (switching supplies)Boost / buck converters store energy in inductor briefly during one phase, release during anotherUSB-C chargers, laptop adapters, EV chargers, solar inverters
Surge limiterSlows the rise of fault current — gives breakers time to interruptSeries reactors at substations, PV string fuses
Solenoid / contactor coilMagnetic field pulls a metal armature → mechanical motionRelays, contactors, valves, actuators

Other Useful Metaphors

Power Triangle = Beer Glass

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Beer = real power; foam = reactive; full glass = apparent
You order a beer, you want to drink the BEER (real power, kW). The FOAM on top (reactive, kVAR) doesn't quench thirst — but it takes up volume. Your bartender pours into a 16 oz glass — the FULL GLASS volume is what they bill (apparent power, kVA). PF = beer / total glass. You want PF as close to 1.0 as possible — pure beer, no foam.

Reactive Power = Dancers Spinning vs Walking

Real power = dancers walking forward (actually getting somewhere). Reactive power = dancers spinning in place (using energy, not progressing). Both look like effort. Only one delivers useful work to the destination.

Resonance = Pushing a Swing

Push at the wrong rhythm: nothing happens, swing barely moves. Push at the natural frequency: swing climbs higher and higher. Same with electrical resonance — when source frequency matches LC natural frequency, current builds dramatically. Why power-factor caps + system inductance can blow up if not detuned (§15).

Transformers = Gear Ratios

Step-up transformer: like a gearbox in low gear. High torque (high current) on input, fast spin (high voltage) on output. Step-down: opposite. Conservation of energy = conservation of (V × I) = conservation of "horsepower" through the gearbox.

3-Phase = 3 Horses Pulling at Even Spacing

Three horses harnessed to a wagon at 120° angular spacing. Each pulls in a different direction. Combined force is constant in magnitude — wagon experiences smooth pull. Single-phase = one horse — pull pulses from full to zero each step. Why 3φ motors are smooth, 1φ motors vibrate.

Grounding = Dump Valve in a Fish Tank

Your fish tank has water at a specific level. Excess pressure (voltage) needs to escape somewhere. The dump valve = ground. Connects tank to the outside (earth). Earth is so big it can absorb anything without changing level. Why we ground every metal enclosure to earth.

Selective Coordination = Falling Dominoes Backwards

Tip the closest domino — it falls. None of the dominoes upstream fall. That's selectivity: only the device closest to the fault opens. The trick is getting the timing right so upstream doesn't beat downstream to falling.

Arc Flash = Fireworks at Point Blank

A small ignition (electrical fault) becomes massive plasma in microseconds. The energy was already there in the system (fault current); the fault just released it. Hence the equation: I × t = energy. Reduce trip time t (mitigation) and you reduce the explosion.

Power Factor = Pulling a Sled at an Angle

Imagine pulling a sled with a rope. Pull straight ahead: 100% of effort goes to motion (PF = 1.0). Pull at 45° angle: half your effort lifts the sled (wasted motion = reactive), half pulls it forward (real). Power factor = cos(angle) of your pull.

Harmonics = Musical Overtones

A pure sine wave is one note. Add overtones (3rd, 5th, 7th harmonics) and the wave gets distorted — instead of a clean note, you get a chord-like buzzy waveform. VFDs, LEDs, server PSUs all generate harmonics. Equipment hates them: motors overheat from negative-sequence currents (5th harmonic), transformers see neutral overload (3rd harmonic = triplens).

Δ Configuration = Triangle Marketplace

3 sellers in a triangle, each connected to the other two. No central authority. Three transactions in three pairs. No neutral exists.

Y (Wye) Configuration = Spoke Wheel

3 sellers all connected to one central hub (the neutral). Each can sell directly to the center, or to neighbors via the center. Neutral provides a reference point — single-phase voltages can be measured to neutral.

Impedance = Walking Through Different Mediums

Walking through air = low resistance + low reactance = low impedance. Walking through water = higher resistance. Walking through a strong wind blowing in your face = reactance (you fight against it) — and the harder the wind blows (the higher the frequency), the more you fight. Capacitors are like walking with a tailwind that pushes you faster than you'd walk in still air.

Fault Current = Flash Flood

Normally water (current) trickles through pipes (conductors) at a measured rate. A burst pipe (short circuit) creates a flash flood — water everywhere, finding the path of least resistance, doing damage. The "flood gates" (breakers) need to slam shut FAST.

Magnetic Field Basics — How Motors Work

  1. Current creates magnetic field. A wire carrying current is surrounded by a circular magnetic field (right-hand rule). Coil the wire → magnetic field becomes a "bar magnet" with N + S poles.
  2. Magnetic field exerts force on a current-carrying wire. If you put a current-carrying wire in another magnetic field, the two fields push the wire perpendicular to both (F = I × L × B).
  3. Combine the two: a stator (stationary winding) creates a magnetic field. A rotor (moving winding or magnet) sits inside the stator and feels force → rotor spins. This is a motor.
  4. Spin a rotor in reverse — get a generator. Mechanical input → magnetic field changes around rotor → induces voltage in stator → output power.
  5. 3-phase magic: three windings 120° apart in space, fed by 3-phase currents 120° apart in time, create a smoothly rotating magnetic field that drags the rotor along. This is why 3-phase induction motors are self-starting.

The Power System Hierarchy

LevelVoltageWhat happens hereWhere in Atlas DC1
Generation13.8 kV typical (at the generator)Hydro, gas, nuclear, wind, solar generators produce electricityThe utility's plants — not on Atlas DC1 site
Transmission69 - 765 kVLong-distance bulk power transfer. Step up to high voltage to minimize I²R losses over hundreds of miles.
Sub-transmission34.5 - 69 kVIntermediate distribution from transmission substations to local distribution substations
Primary distribution4.16 - 34.5 kV (12.47 kV most common)From distribution substation to neighborhoods/customers. Customer's MV service feeders.Atlas DC1 utility service: 12.47 kV
Secondary distribution120/240V (residential), 480Y/277V (commercial)Service transformer step-down to utilization voltageAtlas DC1 480Y/277V main bus
Utilization120, 208, 240, 277, 415, 480VThe voltage your equipment runs onLighting (277V), receptacles (120V), motors (480V), IT (415Y/240V)

Generator → Wall Outlet — One Joule's Journey

  1. Coal/gas/nuclear/water turns a turbine. Turbine spins a 60 Hz synchronous generator at 13.8 kV.
  2. Step-up transformer brings it to 230 kV for transmission.
  3. Power flows hundreds of miles via overhead transmission lines.
  4. Substation step-down: 230 kV → 69 kV sub-transmission.
  5. Distribution substation: 69 kV → 12.47 kV primary distribution.
  6. Neighborhood pole-mount transformer: 12.47 kV → 120/240V single-phase to your house. (Or → 480Y/277V three-phase to a commercial building.)
  7. Inside the building: panelboard → branch circuit → wall outlet.
  8. Your laptop charger: 120V AC → AC-DC → DC-DC → 19V DC at the laptop.

Total efficiency from fuel to laptop: about 30%. (Most loss at the power plant — thermodynamic limits.) Transmission + distribution losses combined are typically only 5-10%.

Where to Go Next

Now that the theory is in place:

  • If you're new to design: read §01 (Conversions) → §02 (How Design Starts) → §03 (Load Analysis). The formulas will make sense, not just be memorized.
  • If you have an EE degree but it's been a while: skim §01, focus on §04 (Branch Circuits) onward.
  • If you're studying for the PE Power exam: the parent has exam-focused practice with the same notation conventions.

Theory primer · The "why" behind the "what" · Skip if you have an EE background

What you can do after this section
  1. Read §01 formulas without memorizing — you'll see the physics behind them.
  2. Explain to a non-EE colleague why AC won, why three-phase exists, and what reactive power physically is.
  3. Draw a phasor for any unbalanced load, and recognize ELI/ICE in any L or C circuit.
Also see