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Electrical engineering basics: 50 core concepts

The basics of electrical engineering: Ohm’s and Kirchhoff’s laws, series and parallel circuits, capacitors, inductors, AC, components and safety.

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Electric charge: symbol and unit

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  1. 1
    Electric charge: symbol and unit
    QQ, measured in coulombs (C)
    An electron carries −1.602×10−19 C-1.602 \times 10^{-19}\ \mathrm{C}, so one coulomb is about 6.24×10186.24 \times 10^{18} electrons.
  2. 2
    Electric current
    The rate of flow of charge: I=QtI = \dfrac{Q}{t}, measured in amperes (A)
    1 A=1 C/s1\ \mathrm{A} = 1\ \mathrm{C/s}
  3. 3
    Voltage (potential difference)
    The work done per unit charge in moving charge between two points: V=WQV = \dfrac{W}{Q}, measured in volts (V)
    1 V=1 J/C1\ \mathrm{V} = 1\ \mathrm{J/C}
  4. 4
    Resistance
    Opposition to current: R=VIR = \dfrac{V}{I}, measured in ohms (Ω\Omega)
    Its reciprocal is conductance, G=1/RG = 1/R, measured in siemens (S).
  5. 5
    Conventional current vs electron flow
    Conventional current flows from positive to negative through the external circuit; electrons drift the opposite way
    Circuit diagrams and the arrows in component symbols use conventional current.
  6. 6
    SI prefixes k, M and G
    Kilo 10310^3, mega 10610^6, giga 10910^9
    Capital M is mega and lowercase m is milli: 4.7 MΩ=4 700 000 Ω4.7\ \mathrm{M\Omega} = 4\,700\,000\ \Omega.
  7. 7
    SI prefixes m, µ, n and p
    Milli 10−310^{-3}, micro 10−610^{-6}, nano 10−910^{-9}, pico 10−1210^{-12}
    Example: 100 nF=0.1 μF=100 000 pF100\ \mathrm{nF} = 0.1\ \mathrm{\mu F} = 100\,000\ \mathrm{pF}.
  8. 8
    Kilowatt-hour (kWh)
    The energy used by 1 kW1\ \mathrm{kW} for one hour: 3.6 MJ3.6\ \mathrm{MJ}
    Energy is power times time, E=PtE = Pt: a 2 kW2\ \mathrm{kW} heater running for 3 hours uses 6 kWh6\ \mathrm{kWh}.
  9. 9
    Ohm’s law
    V=IRV = IR
    It holds for ohmic conductors such as resistors at a constant temperature. Diodes and filament lamps are non-ohmic.
  10. 10
    Electric power
    P=VI=I2R=V2RP = VI = I^2R = \dfrac{V^2}{R}
    Measured in watts: 1 W=1 J/s1\ \mathrm{W} = 1\ \mathrm{J/s}.
  11. 11
    Kirchhoff’s current law (KCL)
    The total current flowing into a node equals the total current flowing out
    It follows from conservation of charge.
  12. 12
    Kirchhoff’s voltage law (KVL)
    The voltages around any closed loop sum to zero
    It follows from conservation of energy.
  13. 13
    Resistance of a wire
    R=ρLAR = \dfrac{\rho L}{A}
    ρ\rho is the resistivity, LL the length and AA the cross-sectional area. Copper’s resistivity is about 1.7×10−8 Ω m1.7 \times 10^{-8}\ \Omega\,\mathrm{m} at 20 °C.
  14. 14
    Terminal voltage of a battery
    V=E−IrV = \mathcal{E} - Ir
    E\mathcal{E} is the EMF and rr the internal resistance, so the voltage sags as the current II rises.
  15. 15
    Resistors in series
    Req=R1+R2+⋯R_{\text{eq}} = R_1 + R_2 + \cdots
    The same current flows through each one, and their voltages add up.
  16. 16
    Resistors in parallel
    1Req=1R1+1R2+⋯\dfrac{1}{R_{\text{eq}}} = \dfrac{1}{R_1} + \dfrac{1}{R_2} + \cdots
    Each has the same voltage across it, and the total is less than the smallest resistance.
  17. 17
    Two resistors in parallel (shortcut)
    Req=R1R2R1+R2R_{\text{eq}} = \dfrac{R_1 R_2}{R_1 + R_2}
    Product over sum. Two equal resistors give half the value: 10 kΩ∥10 kΩ=5 kΩ10\ \mathrm{k\Omega} \parallel 10\ \mathrm{k\Omega} = 5\ \mathrm{k\Omega}.
  18. 18
    Voltage divider
    Vout=Vin R2R1+R2V_{\text{out}} = V_{\text{in}}\,\dfrac{R_2}{R_1 + R_2}
    VoutV_{\text{out}} is taken across R2R_2. It holds only while the load draws negligible current.
  19. 19
    Current divider (two resistors)
    I1=I R2R1+R2I_1 = I\,\dfrac{R_2}{R_1 + R_2}
    The larger share of the current flows through the smaller resistance.
  20. 20
    Resistor colour code: digits 0 to 9
    Black 0, brown 1, red 2, orange 3, yellow 4, green 5, blue 6, violet 7, grey 8, white 9
    The colours from red to violet follow the order of the rainbow.
  21. 21
    Resistor tolerance bands: gold and silver
    Gold ±5%, silver ±10%
    Precision resistors use brown (±1%) or red (±2%).
  22. 22
    Value of a resistor banded brown, black, red, gold
    1 kΩ1\ \mathrm{k\Omega} ±5%
    Brown 1 and black 0 give 10, and the red multiplier band means ×102\times 10^2: 10×100=1000 Ω10 \times 100 = 1000\ \Omega.
  23. 23
    Ceramic capacitor marked 104
    100 nF100\ \mathrm{nF} (0.1 μF0.1\ \mathrm{\mu F})
    The first two digits are the value and the third is the number of zeros, in picofarads: 10×104 pF10 \times 10^4\ \mathrm{pF}.
  24. 24
    Capacitance
    C=QVC = \dfrac{Q}{V}, measured in farads (F)
    A capacitor stores energy in the electric field between two conductors separated by an insulator.
  25. 25
    Energy stored in a capacitor
    E=12CV2E = \tfrac{1}{2}CV^2
  26. 26
    Capacitors in series and in parallel
    Parallel: Ceq=C1+C2+⋯C_{\text{eq}} = C_1 + C_2 + \cdots. Series: 1Ceq=1C1+1C2+⋯\dfrac{1}{C_{\text{eq}}} = \dfrac{1}{C_1} + \dfrac{1}{C_2} + \cdots
    The opposite of the rules for resistors.
  27. 27
    Current through a capacitor
    i=C dvdti = C\,\dfrac{dv}{dt}
    A capacitor passes current only while the voltage across it is changing.
  28. 28
    Voltage across an inductor
    v=L didtv = L\,\dfrac{di}{dt}
    Inductance is measured in henries (H). An inductor stores energy in its magnetic field.
  29. 29
    Energy stored in an inductor
    E=12LI2E = \tfrac{1}{2}LI^2
  30. 30
    Capacitors and inductors in a DC circuit at steady state
    A capacitor acts as an open circuit; an inductor acts as a short circuit
    Nothing is changing, so no current flows into the capacitor and no voltage appears across the inductor.
  31. 31
    Electrolytic capacitors
    They are polarized: the lead marked negative must be at the lower voltage
    Connected in reverse or over their rated voltage, they can overheat, vent or burst.
  32. 32
    AC vs DC
    Direct current flows in one direction only; alternating current reverses direction periodically, usually as a sine wave
    Batteries supply DC; the mains supply is AC.
  33. 33
    Frequency and period
    f=1Tf = \dfrac{1}{T}
    Frequency is measured in hertz (cycles per second): a 50 Hz50\ \mathrm{Hz} wave has a period of 20 ms20\ \mathrm{ms}.
  34. 34
    Mains frequency
    50 Hz50\ \mathrm{Hz} in most of the world; 60 Hz60\ \mathrm{Hz} in North America and some other countries
    Japan uses both: 50 Hz in the east and 60 Hz in the west.
  35. 35
    RMS value of a sine wave
    Vrms=Vpeak2≈0.707 VpeakV_{\text{rms}} = \dfrac{V_{\text{peak}}}{\sqrt{2}} \approx 0.707\,V_{\text{peak}}
    The RMS value is the DC voltage that would heat a resistor at the same average rate.
  36. 36
    Peak voltage of 230 V mains
    About 325 V325\ \mathrm{V} (2302230\sqrt{2})
    Mains voltages are quoted as RMS values. For 120 V mains the peak is about 170 V.
  37. 37
    Diode
    Lets current flow from anode to cathode and blocks it in the reverse direction
    In the symbol the arrow points the way conventional current flows, and the bar marks the cathode.
  38. 38
    Forward voltage of a silicon diode
    About 0.60.6 to 0.7 V0.7\ \mathrm{V}
    Schottky diodes drop less, typically about 0.2 to 0.4 V.
  39. 39
    Series resistor for an LED
    R=Vs−VFIFR = \dfrac{V_s - V_F}{I_F}
    VsV_s is the supply, VFV_F the LED’s forward voltage (about 2 V2\ \mathrm{V} for red, 3 V3\ \mathrm{V} for blue or white) and IFI_F the current, often 1010 to 20 mA20\ \mathrm{mA}.
  40. 40
    Terminals of a BJT and a MOSFET
    BJT: base, collector, emitter. MOSFET: gate, drain, source
    The base and the gate are the control terminals.
  41. 41
    Transistor used as a switch
    A small signal at the base or gate turns a much larger current between the other two terminals fully on or fully off
    A BJT is driven by base current; a MOSFET by gate voltage, with almost no steady gate current.
  42. 42
    Relay
    An electrically operated switch: current through a coil moves a set of contacts
    It lets a small circuit control a separate, isolated circuit at a higher voltage or current.
  43. 43
    Flyback diode across a relay coil
    It gives the coil’s current a path when the coil is switched off, preventing a voltage spike that could destroy the driving transistor
    It is fitted reverse-biased, so it carries no current while the coil is energized.
  44. 44
    Fuse
    A thin conductor that melts and breaks the circuit when the current exceeds its rating
    It protects the wiring from overheating. A circuit breaker does the same job and can be reset.
  45. 45
    How to connect an ammeter and a voltmeter
    An ammeter goes in series with the component; a voltmeter goes in parallel across it
    An ideal ammeter has zero resistance and an ideal voltmeter infinite resistance, so neither disturbs the circuit.
  46. 46
    Short circuit vs open circuit
    A short circuit is a path of almost zero resistance (no voltage across it); an open circuit is a break (no current through it)
  47. 47
    Ground in a circuit diagram
    The reference node, defined as 0 V, that other node voltages are measured from
    It need not be connected to the earth; protective earth is a separate safety connection.
  48. 48
    Protective earth
    A conductor connecting exposed metal parts of equipment to earth, so a fault makes a large current flow and blows the fuse or trips the breaker instead of leaving the case live
  49. 49
    Residual-current device (RCD or GFCI)
    Cuts the supply when the currents in the live and neutral conductors differ, meaning current is leaking to earth, possibly through a person
    Typical trip thresholds are 30 mA for an RCD and about 5 mA for a GFCI.
  50. 50
    Mains wire colours (IEC)
    Brown: live. Blue: neutral. Green and yellow: protective earth
    In North America, black (or red) is hot, white is neutral and green or bare copper is ground.

Frequently asked questions

Do I need calculus for this deck?

Hardly. Nearly every card uses algebra; only the capacitor and inductor equations use derivatives, which you will meet in any first circuits course.

Why do capacitors combine the opposite way to resistors?

Capacitors in parallel act like one capacitor with a larger plate area, so their capacitances add. In series, each one holds the same charge while their voltages add, so the reciprocals add.

What should I learn after this deck?

The intermediate deck moves on to circuit analysis: Thevenin and Norton equivalents, transients, phasors, AC and three-phase power, op-amps, transistors and digital logic.

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