Electrical Theory Foundations
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.
- The Three Quantities + Ohm's Law — voltage, current, resistance, the foundational equation.
- Kirchhoff's Laws (KVL + KCL) — how voltage adds around loops; how current splits at nodes.
- DC vs AC + The Sinusoid — why we use AC; what RMS means.
- Why Three-Phase Is the Standard + The Magic of Transformers — the two ideas that built the grid.
- 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
| Quantity | Symbol | Unit | Plumbing analogy | Elevator analogy | What it physically is |
|---|---|---|---|---|---|
| Voltage | V | Volt (V) | Water pressure between inlet and outlet (PSI) | Floor-to-floor height difference — the up/down journey the elevator delivers | Electrical potential difference between two points — the "push" that wants to move charge. |
| Current | I | Ampere (A) | Water flow rate through a pipe (gal/min) | People riding — when multiple elevators serve the same floors, the crowd splits among them | Charge flowing per second (coulombs per second). Read with a clamp meter on a single conductor. |
| Resistance | R | Ohm (Ω) | Pipe friction — narrower or longer pipe opposes flow more | Slow elevator, long door dwell, queue at the lobby — what limits how many can ride per minute | Opposition to current flow. Depends on conductor size, length, and material. |
| Power | P | Watt (W) | Water power: pressure × flow (PSI × GPM) | People × floors per minute being moved | Rate of energy transfer. P = V × I. |
| Energy | E | Watt-hour (Wh) | Total water moved over time | Total people × floors moved over the day | Power × 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.
Kirchhoff's Laws — How Current and Voltage Behave in Circuits
| Law | Statement | What it means in practice |
|---|---|---|
| KVL — Kirchhoff's Voltage Law | Sum of voltages around any closed loop = 0 | Voltage 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 Law | Sum of currents entering a node = sum of currents leaving | Current splits at a junction in proportion to inverse impedance. Why parallel branches share current. Why neutral current is the unbalanced sum of phase currents. |
DC vs AC — Why We Use Alternating Current
| DC (Direct Current) | AC (Alternating Current) | |
|---|---|---|
| Direction of flow | One direction, constant | Reverses 60 times per second (US) or 50 (Europe) |
| Voltage transformation | Hard — requires DC-DC converters (inefficient at scale) | Easy — passive transformer steps up/down with ~ 99% efficiency |
| Long-distance transmission | Lossy at low voltage; requires HVDC for long distance (specialized + expensive) | Easy — step up to MV/HV, transmit, step down. I²R losses minimized. |
| Where used | Batteries, electronics, telecom, EV traction | Everything 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
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:
| Property | Why 3-phase wins |
|---|---|
| Constant total instantaneous power | P1(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 transmission | 3 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 motors | 3-phase produces a uniform rotating magnetic field. Motor starts on its own. (1-phase motors need start capacitors or shaded poles.) |
| Neutral can be omitted | Balanced 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:
- AC current in primary winding creates a changing magnetic flux in the iron core.
- The changing flux induces a voltage in the secondary winding.
- The voltage ratio = the turns ratio: V₁/V₂ = N₁/N₂.
- 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.
Resistance + Inductance + Capacitance — The Three Passive Elements
| Element | Symbol | What it does | How it acts in AC | Phase relationship |
|---|---|---|---|---|
| Resistor | R | Dissipates 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 primary | L | Stores 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 insulator | C | Stores 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.
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.
| Reactance | Formula | Notes |
|---|---|---|
| Inductive (XL) | XL = 2π × f × L | Higher 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.
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.
| Method | Built on | Unknowns you solve for | Best when… |
|---|---|---|---|
| Mesh (loop) analysis | KVL — sum of voltages around each independent loop = 0 | Mesh (loop) currents | Few loops, lots of voltage sources |
| Nodal analysis | KCL — sum of currents into each node = 0 | Node 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.
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
| Configuration | Resistance | Voltage | Current |
|---|---|---|---|
| Series (one path) | Rtotal = R1 + R2 + ... | V splits across each R | Same I through every R |
| Parallel (multiple paths) | 1/Rtotal = 1/R1 + 1/R2 + ... | Same V across every R | I splits inversely to R |
| Two parallel resistors (special case) | Rtotal = (R1 × R2) / (R1 + R2) | — | — |
| Plumbing analogy | Elevator 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).
- 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).
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.
| Equivalent | What it is | How to find |
|---|---|---|
| Thevenin equivalent (Vth, Rth) | Voltage source Vth in SERIES with resistance Rth | Vth = 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 Rn | In = short-circuit current at the terminals. Rn = Rth (same as Thevenin). |
| Conversion | — | Vth = In × Rn · In = Vth / Rth |
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:
| Sequence | Symbol | What it is | When it exists |
|---|---|---|---|
| Positive sequence | V1, I1 | Balanced 3φ rotating ABC | Always present in normal operation |
| Negative sequence | V2, I2 | Balanced 3φ rotating ACB (reverse) | Created by phase-phase faults, single-phasing of motors, unbalanced loads |
| Zero sequence | V0, I0 | 3 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 is | Rate of energy transfer (instantaneous) | Total energy moved over time |
| Unit | Watt = Joule/sec; kW = 1000 W | Watt-hour = 3600 J; kWh = 1000 Wh |
| Plumbing analogy | Flow rate (gal/min) | Total water moved (gallons) |
| Math | — | kWh = kW × hours |
| What you're billed for | Demand charge ($/kW) | Energy charge ($/kWh) |
| Typical magnitudes | House 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 concept | Hill / 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 circuit | A path the ball can roll DOWN and BACK UP (via the source) |
Voltage Exists Without 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
| Battery | Capacitor | |
|---|---|---|
| Metaphor | Worker repeatedly LIFTING the rock back to the top of the hill | Lifting the rock to the top ONCE |
| Mechanism | Chemical reaction continuously moves charges from − to + terminal | Pump charges onto plates against the field; field stores them in place |
| "Dead" state | Chemistry runs out — worker can't lift anymore | Charges flowed back through circuit — rock is back at the bottom |
| Recharge | Reverse the chemical reaction (charging the battery) | Pump charges back onto plates (voltage source charges the cap) |
| Stored energy | Chemical bonds (the worker's stamina) | Electric field between plates (the rock's height) |
| Voltage decay | Stays roughly constant until exhausted, then drops | Drops 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.
| Dimension | Capacitor | Inductor |
|---|---|---|
| Stores energy in | Electric field (between plates) | Magnetic field (around coil) |
| Energy formula | E = ½CV² | E = ½LI² |
| Stores variable | VOLTAGE (V across plates) | CURRENT (I through coil) |
| Resists changes in | Voltage (V can't jump instantly — physics requires charge to accumulate) | Current (I can't jump instantly — physics requires field to build) |
| Physical intuition | Compressing a spring (compressing charge separation) | Spinning a flywheel (storing rotational energy) |
| What happens when source disconnects | Holds voltage (until leakage drains) | Tries to maintain current — generates voltage spike (back-EMF) |
| "Open circuit" version | No effect — already open | Cap-like: holds whatever charge the field had |
| "Short circuit" version | Discharges fast through wire | No effect — already short |
The Flywheel Intuition for Inductors
Imagine a heavy flywheel on bearings:
| Action | Flywheel | Inductor |
|---|---|---|
| Apply force / voltage | Slowly accelerates — won't spin instantly | Current rises slowly — voltage causes I to ramp up over time |
| Stop pushing | Keeps spinning by inertia | Current 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 friction | Stored energy released as heat in resistance |
Charging + Discharging — Time Curves
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:
- Current flows TOWARD the cap (charging up).
- As charge accumulates, voltage rises BEHIND the current.
- When voltage peaks, current has already started to reverse (charge is starting to leave).
- 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:
- Voltage rises across the coil.
- Current builds slowly behind it.
- When current peaks, voltage has already started decreasing.
- Voltage LEADS current by 90°.
Memory aid: "ELI" — in an inductor (L), voltage (E) leads current (I). Together: "ELI the ICE man" covers both.
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
| Application | What the cap does | Where you see it |
|---|---|---|
| Filter cap (DC supplies) | Smooths ripple after rectifier — caps charge during peaks, release during dips | Every wall-wart, every PSU. Big electrolytic on the rail. |
| Coupling cap | Blocks DC offset, passes AC fluctuation | Audio amplifiers, sensor signal chains |
| Decoupling / bypass cap | Local current reservoir for fast IC switching — keeps voltage stable when chip suddenly draws current | Every digital IC has 100 nF caps next to it |
| Power factor correction | Cap supplies reactive current locally — cancels inductive lag from motors | Industrial PFC banks (§14, §15) |
| Tuned circuit (with inductor) | L and C resonate at specific frequency — extracts that frequency from a signal | Radio receivers, harmonic filters, RF impedance matching |
| Energy storage (pulsed apps) | Stores energy slowly, releases burst quickly | Camera flash, defibrillator, Tesla coils, UPS DC bus, particle accelerators |
| Snubber circuit | Absorbs voltage spikes during inductive switching | Across relay contacts, in motor drives |
| Timing circuit (with R) | RC time constant τ = R·C controls how fast V changes | 555 timers, retriggerable monostables, debouncers |
| Motor starting (split-phase) | Cap creates a phase-shifted second winding — gives 1φ motor a starting torque | Single-phase induction motors (HVAC compressors, well pumps) |
Why Inductors Are Used in Real Circuits
| Application | What the inductor does | Where you see it |
|---|---|---|
| Filter inductor (choke) | Smooths CURRENT ripple — opposite of cap which smooths voltage | Audio amp output, switching power supply output, VFD output reactor |
| Current-limiting reactor | Series inductance limits inrush current | Soft-start motor drives, MV switchgear sub-transient current limiting |
| Transformer winding | Creates the magnetic flux that couples primary to secondary | Every transformer (§09) |
| Motor / generator winding | Creates the rotating field that produces torque (or extracts torque) | Every electric motor + generator |
| Tuned circuit (with cap) | L and C resonate at specific frequency | Radio receivers, harmonic filters |
| EMI filter | Inductor 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 another | USB-C chargers, laptop adapters, EV chargers, solar inverters |
| Surge limiter | Slows the rise of fault current — gives breakers time to interrupt | Series reactors at substations, PV string fuses |
| Solenoid / contactor coil | Magnetic field pulls a metal armature → mechanical motion | Relays, contactors, valves, actuators |
Other Useful Metaphors
Power Triangle = Beer Glass
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
- 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.
- 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).
- 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.
- Spin a rotor in reverse — get a generator. Mechanical input → magnetic field changes around rotor → induces voltage in stator → output power.
- 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
| Level | Voltage | What happens here | Where in Atlas DC1 |
|---|---|---|---|
| Generation | 13.8 kV typical (at the generator) | Hydro, gas, nuclear, wind, solar generators produce electricity | The utility's plants — not on Atlas DC1 site |
| Transmission | 69 - 765 kV | Long-distance bulk power transfer. Step up to high voltage to minimize I²R losses over hundreds of miles. | — |
| Sub-transmission | 34.5 - 69 kV | Intermediate distribution from transmission substations to local distribution substations | — |
| Primary distribution | 4.16 - 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 distribution | 120/240V (residential), 480Y/277V (commercial) | Service transformer step-down to utilization voltage | Atlas DC1 480Y/277V main bus |
| Utilization | 120, 208, 240, 277, 415, 480V | The voltage your equipment runs on | Lighting (277V), receptacles (120V), motors (480V), IT (415Y/240V) |
Generator → Wall Outlet — One Joule's Journey
- Coal/gas/nuclear/water turns a turbine. Turbine spins a 60 Hz synchronous generator at 13.8 kV.
- Step-up transformer brings it to 230 kV for transmission.
- Power flows hundreds of miles via overhead transmission lines.
- Substation step-down: 230 kV → 69 kV sub-transmission.
- Distribution substation: 69 kV → 12.47 kV primary distribution.
- Neighborhood pole-mount transformer: 12.47 kV → 120/240V single-phase to your house. (Or → 480Y/277V three-phase to a commercial building.)
- Inside the building: panelboard → branch circuit → wall outlet.
- 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
- Read §01 formulas without memorizing — you'll see the physics behind them.
- Explain to a non-EE colleague why AC won, why three-phase exists, and what reactive power physically is.
- Draw a phasor for any unbalanced load, and recognize ELI/ICE in any L or C circuit.