Junction Potential: Nichrome Wires of Different Lengths & Areas

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SUMMARY

The discussion centers on calculating the junction potential between two nichrome wires of differing lengths and cross-sectional areas. The longer wire, measuring 2L with area A, is connected to a shorter wire of length L and area 2A. Given the electric potentials of 8.0 V at the free end of the longer wire and 1.0 V at the shorter wire, the potential at the junction can be determined by analyzing the potential drop across each wire. The key conclusion is that the potential difference is not uniform due to the variable cross-sectional area, which introduces resistance characteristics in the wires.

PREREQUISITES
  • Understanding of electric potential and voltage in circuits
  • Knowledge of Ohm's Law and resistance in conductors
  • Familiarity with the concept of equipoential surfaces in conductors
  • Basic principles of series circuits and potential drops across components
NEXT STEPS
  • Study the relationship between resistance and cross-sectional area in conductors
  • Learn about potential drop calculations in series circuits
  • Explore the concept of variable resistors and their applications
  • Investigate the properties of nichrome as a resistive material in electrical applications
USEFUL FOR

Students studying electrical engineering, physics enthusiasts, and anyone interested in understanding the behavior of electrical circuits involving resistive materials.

jdstokes
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Homework Statement



One end of a nichrome wire of length 2L and cross-sectional area A is attached to an end of another nichrome wire of length L and cross-sectional area 2A. If the free end of the longer wire is at an electric potential of 8.0 V, and the free end of the shorter wire is at an electric potential of 1.0 V, the potential at the junction of the two wires is equal to

The Attempt at a Solution



I have conceptual problems with this question. In an ordinary piece of `circuit wire' it is impossible to maintain a nonzero potential difference between each end. Does this mean that a wire with variable width behaves as a kind of resistor? Would the potential difference not be everywhere the same because of equipoential on a conductor?
 
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I was missing the point, the idea is to compute the potential drop across one component, as a fraction of the total potential drop. Knowing the absolute potentials at the ends allows the junction potential to be calculated.
 

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