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United StatesPhysics C: Electricity and MagnetismSyllabus dot point

How do resistance and resistivity arise, and what does Ohm's law say about them?

Topic 11.3 Resistance, Resistivity, and Ohm's Law: relate resistance to resistivity and geometry, apply Ohm's law, and distinguish ohmic from non-ohmic behavior.

A calculus-based answer to AP Physics C E&M Topic 11.3, covering Ohm's law, resistance from resistivity and geometry, the microscopic form J = sigma E, temperature dependence, and ohmic versus non-ohmic devices.

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  1. What this topic is asking
  2. Ohm's law and resistance
  3. Resistance from resistivity and geometry
  4. The microscopic form and temperature
  5. Try this

What this topic is asking

The College Board (Topic 11.3) wants you to relate resistance to resistivity and geometry, apply Ohm's law V=IRV = IR, understand its microscopic form J=σE\vec{J} = \sigma\vec{E}, and distinguish ohmic from non-ohmic devices. Resistance is what opposes current and converts electrical energy to heat.

Ohm's law and resistance

Resistance measures how strongly a conductor opposes current: for a given voltage, a higher RR allows less current. Ohm's law is an empirical relation, not a fundamental law, and holds for metals over a wide range but not for every device.

Resistance from resistivity and geometry

The resistance of a uniform conductor depends on the material and its shape:

R=ρLAR = \frac{\rho L}{A}

where ρ\rho is the resistivity (an intrinsic property of the material, in Ω\Omega\,m), LL the length, and AA the cross-sectional area. A longer wire has more resistance; a thicker wire has less. Resistivity ranges over many orders of magnitude, from good conductors (copper, 108Ω\sim10^{-8}\,\Omega\,m) to insulators (1016Ω\sim10^{16}\,\Omega\,m).

The microscopic form and temperature

At the level of the current density and field, Ohm's law reads

J=σE,σ=1ρ\vec{J} = \sigma\vec{E}, \qquad \sigma = \frac{1}{\rho}

with σ\sigma the conductivity. This says the local current density is proportional to the local field. In a metal, resistivity rises with temperature because hotter ions vibrate more and scatter the drifting electrons more often:

ρ=ρ0[1+α(TT0)]\rho = \rho_0\left[1 + \alpha(T - T_0)\right]

where α\alpha is the temperature coefficient.

Try this

Q1. A resistor obeys Ohm's law with R=20ΩR = 20\,\Omega. Find the current at 1010 V. [2 points]

  • Cue. I=VR=1020=0.50I = \dfrac{V}{R} = \dfrac{10}{20} = 0.50 A.

Q2. State how the II-VV graph of an ohmic resistor looks. [1 point]

  • Cue. A straight line through the origin (constant slope 1/R1/R).

Exam-style practice questions

Practice questions written in the style of College Board exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

AP 2023 (style)1 marksSection I (multiple choice). A wire of resistance RR is stretched to twice its length while its volume stays constant. Its new resistance is (A) RR (B) 2R2R (C) 4R4R (D) R/2R/2. Justify your reasoning.
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A 1-point MCQ on resistance and geometry. The answer is (C).

R=ρLAR = \dfrac{\rho L}{A}. Doubling LL at constant volume halves AA (since V=LAV = LA is fixed). So Rρ2LA/2=4ρLA=4RR \to \rho\dfrac{2L}{A/2} = 4\dfrac{\rho L}{A} = 4R. The trap is (B): only the length is considered, missing that the cross-section also shrinks.

AP 2024 (style)4 marksSection II (FRQ, quantitative and conceptual). A cylindrical resistor has length 0.500.50 m, cross-sectional area 1.0×1061.0\times10^{-6} m squared, and resistivity 5.0×107Ωm5.0\times10^{-7}\,\Omega\,\text{m}. (a) Calculate its resistance. (b) If 3.03.0 V is applied, calculate the current. (c) State what distinguishes an ohmic from a non-ohmic device on an II-VV graph.
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A 4-point FRQ on resistance and Ohm's law.

(a) Resistance (2 points): R=ρLA=(5.0×107)(0.50)1.0×106=0.25ΩR = \dfrac{\rho L}{A} = \dfrac{(5.0\times10^{-7})(0.50)}{1.0\times10^{-6}} = 0.25\,\Omega.
(b) Current (1 point): I=VR=3.00.25=12I = \dfrac{V}{R} = \dfrac{3.0}{0.25} = 12 A.
(c) Ohmic vs non-ohmic (1 point): an ohmic device gives a straight line through the origin on an II-VV graph (constant RR); a non-ohmic device (a diode, a filament bulb) gives a curved line, so RR changes with voltage.

Markers reward R=ρL/AR = \rho L/A, Ohm's law, and the straight-versus-curved distinction.

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