How to Calculate Heat Generated by Electric Current in Different Materials?

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Discussion Overview

The discussion revolves around calculating the heat generated by electric current in various materials, particularly focusing on different scenarios such as aqueous solutions and battery cells. Participants explore theoretical and practical aspects of heat generation, resistance behavior, and material properties.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how to determine heat generation from current, noting the use of the formula I²R and its applicability to aqueous materials and large battery cells.
  • Another participant suggests that while I²R can be used for aqueous solutions, resistance may not remain constant, proposing that voltage times current might be a better approach for practical measurement.
  • There is a discussion about the heating effects in batteries, attributed to internal resistances and chemical processes, with a method proposed for measuring internal resistance through terminal voltage drop.
  • A participant raises the idea of minimizing heat generation by selecting materials that decrease resistance with current, while maximizing heat would involve materials that increase resistance.
  • Another participant counters this by suggesting the use of materials with opposite temperature coefficients in series to achieve a more constant resistance, referencing historical examples of filament behavior in lamps and transistors.
  • A later post poses a theoretical question about maximizing heat generation in a super electric heater, considering voltage and amperage over time, without specifying engineering limitations.

Areas of Agreement / Disagreement

Participants express differing views on the best methods for calculating and maximizing heat generation, with no consensus reached on the most effective approach or the implications of resistance behavior in various materials.

Contextual Notes

Participants acknowledge the complexity of resistance behavior in different materials, particularly under varying temperatures and current densities, and the challenges in predicting resistance in aqueous solutions and battery systems.

Frostfire
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Ive posted this a while back but never had a reply,

How does one determine the heat generated from a current? I have found several sources that refer to using "the length of a wire" but how would you calculate it for an aqueous material, or for all intensive purposes a "really large" battery cell. Would = I^2 *R still work?

Also I haven't worked with high current problems before, I remember something about resistance increasing drastically with high current density.
 
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If you were forcing current through an aqueous solution, I squared R would work. However, you couldn't predict R and you wouldn't know if it stayed constant.
So, it would be better to just use voltage times current. You can measure these OK.

There are heating effects in a battery but this is due to internal resistances in the leads to the electrodes, and the electrodes themselves, as well as limits in the chemical processes involved.

You can measure this internal resistance in a battery by loading it and noting the drop in terminal voltage. You could then predict the heating using I squared R.

Resistance in a solid conductor does increase with temperature for most substances, although there are some like Carbon and semiconductors, like Silicon and Germanium, that reduce their resistance with temperature.
 
Interesting, so that brings up another question. If to calculate it in an aqueous solution involves working around resistance. If one was trying to minimize heat, use a material that behaves in a manner decreasing resistance with current, and to maximize use one that does the opposite?, That sound right, if incredibly over simplified
 
No, but you could compensate for the CHANGE in resistance of one substance by using a substance of opposite temperature coefficient with it so that you would get more of a constant resistance.

So, if you had one resistor that increased resistance with temperature, you could put another in series with it that decreased resistance with temperature. This could partly cancel out the change resulting in a more constant total resistance with temperature.

Early (Edison) lamps used carbon filaments. These reduced resistance with temperature, meaning they would draw more current and get hotter. This is a sort of runaway process that could destroy the lamp.
Later lamps used metal filaments that increase resistance with temperature, so they tend to protect themselves by drawing less current when they get hot.
Germanium transistors had the same thermal runaway problem and had to be designed into circuits that stopped this effect causing destruction.
 
Thanks for the reply's, I've been off for a while, you know how it is, out of class and work,try to focus on something else for a bit :wink: I hadn't thought about the thermal balance, interesting concept though,

So theory question, If one was trying to maximize the heat generated by a system, say a super electric heater based on high voltage, baring engineering limitations, what would be the best way to set it up to maximize heat induced from a given voltage, at a given amperage as well if required, over a given time?
 

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