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/Δt. Unit: ampere (A = C/s). Conventional current flows from positive to negative terminal externally — opposite to the direction electrons move.
Resistance and Resistivity
Resistance R (ohms, Ω) opposes current flow. It depends on the material's resistivity ρ (Ω·m), the length L, and cross-sectional area A: R=ρL/A. Longer or thinner conductors have higher resistance.
Ohm's Law
For ohmic (linear) materials, the current is proportional to the applied voltage: V=IR, or equivalently I=V/R. The resistance R is constant regardless of V or I for ohmic devices. Many devices (diodes, bulbs) are non-ohmic.
Temperature Dependence
For most metals, resistivity increases linearly with temperature: R=R0(1+αΔT), where α is the temperature coefficient of resistance (positive for metals, negative for semiconductors) and ΔT=T−T0.
Electric Power
The rate at which a resistor converts electrical energy to heat: P=IV=I2R=V2/R. Unit: watt (W). Energy dissipated over time t: E=Pt.
Key Equations
Electric current
I=ΔtΔQ
Current in amperes equals charge (coulombs) flowing per second.
Resistance from geometry
R=AρL
R in ohms; ρ = resistivity (Ω·m); L = length; A = cross-sectional area.
Ohm's Law
V=IR
Voltage across a resistor equals current times resistance. Valid for ohmic (linear) devices.
Electric power
P=IV=I2R=RV2
Power dissipated in a resistor. Use whichever form matches what is given.
Temperature dependence
R=R0(1+αΔT)
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=1.72×10−8Ω⋅m) has length L=10 m and diameter d=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(0.50×10−3)2=7.85×10−7 m². Resistance:
R=AρL=7.85×10−7(1.72×10−8)(10)=0.219Ω
(b) Current by Ohm's Law:
I=RV=0.2191.5=6.85 A
(c) Power dissipated:
P=IV=(6.85)(1.5)=10.3 W
AnswerR = 0.219 Ω; I = 6.85 A; P = 10.3 W.
Practice
Exercises
7 problems
1of 7
A charge of Q=120 C passes through a wire cross-section in t=2.0 minutes. What is the current (in A)?
A
2of 7
A nichrome wire (ρ=1.10×10−6Ω⋅m) is L=2.0 m long with cross-sectional area A=0.50×10−6 m². What is its resistance (in Ω)?
Ω
3of 7
A 30Ω resistor is connected to a 9.0 V battery. What current (in A) flows through it?
A
4of 7
A current of I=2.0 A flows through a 50Ω resistor. What power (in W) is dissipated?
W
5of 7
A 60 W light bulb operates at V=120 V. What is its operating resistance (in Ω)?
Ω
6of 7
A copper resistor has R0=100Ω at T0=20°C. Copper has α=3.9×10−3/°C. What is its resistance (in Ω) at T=80°C?
Ω
7of 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/A: longer wire → more resistance; thicker wire → less resistance. Resistivity ρ is a material property.
Ohm's law V=IR applies to ohmic devices — the I–V curve is linear. Always check whether a device is truly ohmic.
Power P=I2R shows that doubling the current quadruples the heat generated — relevant for fuse and wire sizing.
Metal resistivity increases with temperature (positive α); semiconductors decrease (negative α) — the basis of thermistors.