Separate resistance geometry from a power claim
Resistance R describes a particular component, whereas resistivity ρ describes a material under specified conditions. For a uniform wire, R=ρL/A. Doubling its length doubles resistance; doubling its cross-sectional area halves resistance. Doubling diameter instead quadruples area for a circular wire, so diameter and area changes must not be confused.
Learning outcome: Compare lengths 1 and 2 m at area 0.20 mm². Record R and both powers, naming the source condition for every ratio. Then halve area and compare the result with doubling length.
Starting recap
Distinguish charge flow from energy transfer. Identify nodes, choose consistent current/voltage signs and state source and initial conditions before applying algebra.
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Try
With ρ=1.0×10⁻⁶ Ω m, L=1 m and A=0.20 mm²=2.0×10⁻⁷ m², R=5 Ω. At 2 V the current is 0.40 A and power 0.80 W. Under the separate fixed 0.20 A condition, power is 0.20 W.
Open the experimentPredict
If length doubles, do the fixed-voltage and fixed-current power predictions have the same sign of change?
Experiment
Compare lengths 1 and 2 m at area 0.20 mm². Record R and both powers, naming the source condition for every ratio. Then halve area and compare the result with doubling length.
Separate material resistivity, geometry and power constraints
Worked teaching model · synthetic values · Hypothetical constant resistivity 1.0×10⁻⁶ Ω m at fixed temperature. Uniform wire; ideal 2 V source. A separate 0.20 A fixed-current comparison is explicitly a different source boundary. No physical heating or short-circuit activity.
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Circuit connections: Ideal 2 V source and one uniform resistive wire in a closed loop; separate fixed-current comparison is not a second simultaneous source.
Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Wire resistance | 5 | Ω |
| Current at fixed 2 V | 0.4 | A |
| Power at fixed 2 V | 0.8 | W |
| Power at fixed 0.20 A | 0.2 | W |
Accessible plot coordinates
| wire length (m) | resistance (Ω) |
|---|---|
| 0.5 | 2.5 |
| 0.75 | 3.75 |
| 1 | 5 |
| 1.25 | 6.25 |
| 1.5 | 7.5 |
| 1.75 | 8.75 |
| 2 | 10 |
Resistance depends on material and geometry; the effect on power depends on what the source holds fixed.
Use R=ρL/A, P=IV, P=V²/R at fixed voltage and P=I²R at fixed current. Material resistivity is held constant here; real metal heating often increases it. These are two different source conditions, not simultaneous constraints.
Resistance depends on material and geometry; the effect on power depends on what the source holds fixed.
Use R=ρL/A, P=IV, P=V²/R at fixed voltage and P=I²R at fixed current. Material resistivity is held constant here; real metal heating often increases it. These are two different source conditions, not simultaneous constraints.
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Public practice checks a specific claim. It does not establish independent mastery.
How would unmeasured heating undermine an inference that resistivity stayed constant?
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