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Circuits overview

Chapter revision

Revision summary

Key ideas, equations and common mistakes. Open any topic below for the full explanation.

Identify the nodes, the component and the stated conditions. Then choose a relationship that uses the correct current, voltage and source model.

Connections and measurements

  • Series components share current along an unbranched path; parallel components share both endpoints and therefore p.d.
  • An ammeter measures current in its own path. A voltmeter measures p.d. between its own terminals. Pair component V with component I before using R = V/I.
  • Check range, resolution, zero, polarity, loading and thermal conditions. Repeated readings assess scatter but do not remove a consistent wrong-endpoint or zero error.

Resistance and material behaviour

R = V/I    R = ρl/A
A = πd2/4
Rseries = R1 + R2 + …
1/Rparallel = 1/R1 + 1/R2 + …

Convert diameter before squaring it. At fixed material, temperature and length, resistance is proportional to 1/A; doubling diameter quarters resistance. On an I-against-V plot, only a straight line through the origin has gradient 1/R at all points.

  • Ohmic resistor: proportional I and V under fixed physical conditions.
  • Filament lamp: settled heating raises resistance, so the I-V curve becomes less steep at greater voltage magnitude.
  • Semiconductor diode: forward conduction and small reverse current before breakdown; no universal forward threshold.
  • NTC thermistor: warming lowers resistance. A self-heated voltage sweep differs from a fixed-temperature, low-field measurement.

For a typical metal at the same electric field, greater scattering lowers mean drift speed while carrier density changes little. For the stated NTC regime, increased carrier number density is the main explanation for falling resistivity. Random thermal motion is not the directed drift.

Sources, networks and outputs

Vterminal = Es - Ir
I = Es/(Rexternal + r)
Pload = IVterminal
Pinternal = I2r
EsI = Pload + Pinternal

These source signs describe current delivered to the load. A terminal-V-against-I line has intercept Es and gradient -r. Maximum load power occurs at Rexternal = r for this fixed source model, where load and internal powers are equal; this is not maximum efficiency.

Reduce a network to find total current, then work back to its branch voltages and currents. After a connection changes, recalculate the complete network: another branch's voltage may change even if its resistance does not.

Unloaded output across the lower arm:
Vout = VsRlower/(Rupper + Rlower)

Use the actual supply-terminal p.d. The selected output determines the numerator. Work through sensor resistance, total current and output rather than memorising a direction. An output load is parallel with its selected arm and changes the effective divider.

Quantity and unit reference

Quantities used in circuit calculations and measurements
QuantitySymbolSI unit
CurrentIA
Potential differenceVV = J/C
Source e.m.f.Es, EV
Resistance; internal resistanceR; rΩ = V/A
ResistivityρΩ m
Length; diameterl; dm
Cross-sectional areaAm2
PowerPW = J/s
ChargeQC = A s
Timets

Read symbols in context: A as area differs from A as the ampere unit, and C as charge's unit differs from a node labelled C. Useful prefixes are micro (µ, 10-6), milli (m, 10-3), kilo (k, 103) and mega (M, 106). Squared lengths and areas require squared conversion factors.

For a calculation, draw or trace the nodes, choose reference directions and endpoints, state the component conditions, solve with units, then check current and energy accounts. For a measurement, retain the actual readings and instrument information as well as the inferred result.

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