NEET 2020 Physics Question 163 Solution
Question
Which of the following graph represents the variation of resistivity (ρ) with temperature (T) for copper?
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Which of the following graph represents the variation of resistivity (ρ) with temperature (T) for copper?
In standard NCERT, resistivity of copper vs temperature in Kelvin is plotted as a non-linear curve starting very low near 0 K and curving upwards (concave upward). Semiconductor resistivity decreases exponentially, alloys like Nichrome have a high non-zero intercept with linear rise, but pure copper displays the curved non-linear rise of Graph (3)!
For metals, resistivity is given by Drude-Lorentz model: , where is the free electron density and is relaxation time. As temperature increases, lattice vibrations (phonons) increase, shortening and increasing .
For pure metals such as copper, at temperatures close to absolute zero ( to ), resistivity increases non-linearly with temperature (proportional to according to quantum electron-phonon scattering theory).
As temperature exceeds , the rate of increase settles into a nearly linear dependence (). Thus the full plot starting from curves upward initially.
- Graph 1: Decreasing exponential (typical of intrinsic semiconductors). - Graph 2: Constant horizontal line (temperature-independent ideal resistor). - Graph 3: Curved upward non-linear plot starting near origin (exact NCERT plot for Copper). - Graph 4: Pure straight line passing through origin (neglects quantum low-temperature non-linearity). Therefore, Graph 3 is the correct representation.
Diagnose every choice: Know exactly why the right option works and why distractors fail.
Incorrect; depicts semiconductor behavior where thermal excitation generates more charge carriers.
Incorrect; depicts a zero temperature coefficient material (ideal standard resistor), not pure copper.
Canonical NCERT curve for copper showing non-linear increase at low T transitioning to linear at higher T.
Incorrect; ignores the well-known low-temperature non-linear curvature in pure copper.
The formula is a linear approximation over narrow temperature ranges. Over the full range from 0 K, the curve is distinctly non-linear.
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