← General Physics II
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Current & Resistance

When a potential difference is maintained across a conductor, charges flow continuously — we call this electric current. The relationship between current, voltage, and the material's resistance is Ohm's law. Understanding how resistance depends on material, geometry, and temperature is essential for every practical circuit, from household wiring to microchips.

Key Concepts

Electric Current
The rate of charge flow past a cross section: I=ΔQ/ΔtI = \Delta Q/\Delta t. Unit: ampere (A = C/s). Conventional current flows from positive to negative terminal externally — opposite to the direction electrons move.
Resistance and Resistivity
Resistance RR (ohms, Ω) opposes current flow. It depends on the material's resistivity ρ\rho (Ω·m), the length LL, and cross-sectional area AA: R=ρL/AR = \rho L/A. Longer or thinner conductors have higher resistance.
Ohm's Law
For ohmic (linear) materials, the current is proportional to the applied voltage: V=IRV = IR, or equivalently I=V/RI = V/R. The resistance RR is constant regardless of VV or II for ohmic devices. Many devices (diodes, bulbs) are non-ohmic.
Temperature Dependence
For most metals, resistivity increases linearly with temperature: R=R0(1+αΔT)R = R_0(1 + \alpha\,\Delta T), where α\alpha is the temperature coefficient of resistance (positive for metals, negative for semiconductors) and ΔT=TT0\Delta T = T - T_0.
Electric Power
The rate at which a resistor converts electrical energy to heat: P=IV=I2R=V2/RP = IV = I^2R = V^2/R. Unit: watt (W). Energy dissipated over time tt: E=PtE = Pt.

Key Equations

Electric current
I=ΔQΔtI = \frac{\Delta Q}{\Delta t}
Current in amperes equals charge (coulombs) flowing per second.
Resistance from geometry
R=ρLAR = \frac{\rho L}{A}
R in ohms; ρ = resistivity (Ω·m); L = length; A = cross-sectional area.
Ohm's Law
V=IRV = IR
Voltage across a resistor equals current times resistance. Valid for ohmic (linear) devices.
Electric power
P=IV=I2R=V2RP = IV = I^2R = \frac{V^2}{R}
Power dissipated in a resistor. Use whichever form matches what is given.
Temperature dependence
R=R0(1+αΔT)R = R_0\bigl(1 + \alpha\,\Delta T\bigr)
R₀ is resistance at reference temperature T₀; α is temperature coefficient (e.g., copper: α ≈ 3.9×10⁻³ /°C).
Worked Example

Resistance, Current, and Power in a Copper Wire

Problem

A copper wire (ρ=1.72×108Ω\rho = 1.72\times10^{-8}\,\Omega\cdotm) has length L=10L = 10 m and diameter d=1.0d = 1.0 mm. Find (a) its resistance, (b) the current if connected to a 1.5 V battery, and (c) the power dissipated.

Solution

(a) Cross-sectional area: A=π(d/2)2=π(0.50×103)2=7.85×107A = \pi(d/2)^2 = \pi(0.50\times10^{-3})^2 = 7.85\times10^{-7} m². Resistance:

R=ρLA=(1.72×108)(10)7.85×107=0.219ΩR = \frac{\rho L}{A} = \frac{(1.72\times10^{-8})(10)}{7.85\times10^{-7}} = 0.219\,\Omega

(b) Current by Ohm's Law:

I=VR=1.50.219=6.85 AI = \frac{V}{R} = \frac{1.5}{0.219} = 6.85\text{ A}

(c) Power dissipated:

P=IV=(6.85)(1.5)=10.3 WP = IV = (6.85)(1.5) = 10.3\text{ W}
Answer R = 0.219 Ω; I = 6.85 A; P = 10.3 W.
Practice

Exercises

7 problems
1 of 7

A charge of Q=120Q = 120 C passes through a wire cross-section in t=2.0t = 2.0 minutes. What is the current (in A)?

A
2 of 7

A nichrome wire (ρ=1.10×106Ω\rho = 1.10\times10^{-6}\,\Omega\cdotm) is L=2.0L = 2.0 m long with cross-sectional area A=0.50×106A = 0.50\times10^{-6} m². What is its resistance (in Ω)?

Ω
3 of 7

A 30Ω30\,\Omega resistor is connected to a 9.09.0 V battery. What current (in A) flows through it?

A
4 of 7

A current of I=2.0I = 2.0 A flows through a 50Ω50\,\Omega resistor. What power (in W) is dissipated?

W
5 of 7

A 60 W light bulb operates at V=120V = 120 V. What is its operating resistance (in Ω)?

Ω
6 of 7

A copper resistor has R0=100ΩR_0 = 100\,\Omega at T0=20°T_0 = 20°C. Copper has α=3.9×103\alpha = 3.9\times10^{-3}/°C. What is its resistance (in Ω) at T=80°T = 80°C?

Ω
7 of 7

A 100 W appliance runs for 3.0 hours. How much energy (in kWh) does it consume?

kWh

Key Takeaways

  • Current is the rate of charge flow; resistance opposes it. Both are needed to predict what happens in a circuit.
  • R=ρL/AR = \rho L/A: longer wire → more resistance; thicker wire → less resistance. Resistivity ρ\rho is a material property.
  • Ohm's law V=IRV = IR applies to ohmic devices — the IIVV curve is linear. Always check whether a device is truly ohmic.
  • Power P=I2RP = I^2R shows that doubling the current quadruples the heat generated — relevant for fuse and wire sizing.
  • Metal resistivity increases with temperature (positive α\alpha); semiconductors decrease (negative α\alpha) — the basis of thermistors.