Understanding Specific Heat: A Derivation of the Correct Equation

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SUMMARY

The discussion focuses on the derivation of the correct equation for specific heat, emphasizing that specific heat, denoted as c(x,u), is a function of both position and temperature. It clarifies that the energy required to raise the temperature of a thin slice from 0° to u(x,t) is represented by the integral of c(x,u') from 0 to u, rather than the product of c(x,u(x,t)) and u(x,t). The conversation highlights the misconception that heat capacity can be treated as a constant, stressing that it is a derivative of internal energy with respect to temperature and varies with temperature changes.

PREREQUISITES
  • Understanding of thermodynamics concepts, particularly specific heat capacity.
  • Familiarity with calculus, specifically integration and differentiation.
  • Knowledge of temperature scales, particularly the Kelvin scale.
  • Basic principles of energy transfer and heat exchange in materials.
NEXT STEPS
  • Study the derivation of the specific heat equation in thermodynamics.
  • Learn about the implications of variable specific heat in thermal analysis.
  • Explore the concept of heat capacity and its relationship to internal energy.
  • Investigate practical applications of specific heat in engineering and material science.
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Students and professionals in physics, engineering, and materials science who are looking to deepen their understanding of specific heat and its mathematical derivation.

FAS1998
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Homework Statement



1.2.6. Supose that the specific heat is a function of position and temperature, c(x,u).

(a)Show that the heat energy per unit mass necesary to raise the temperature of a thin slice of thickness deltax from 0°to u(x,t) is not c(x)u(x,t), but instead int((0->u)c(x,u’))du’.

Homework Equations

The Attempt at a Solution


[/B]
I believe c(x,u) gives the energy per unit mass required to raise the temperature by 1 K as a function in of position and temperature.

And u(x,t) is the temperature as a function of position and time.

So I would’ve thought that the energy per unit mass required to raise the temperature to u(x,t) would be the desired temperature (u(x,t)) multiplied by the specific heat (c(x,u(x,t))).

This would give me u(x,t)c(x,u(x,t))), which is not what they’re looking for, and is very close to what they explicitly say is an incorrect answer.
 
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The heat capacity is not the energy required to raise the temperature by 1 K. It is the energy required to raise the temperature a small amount divided by that small change in temperature. In other words, it is a derivative of internal energy wrt temperature. The multiplication will only hold if the heat capacity is constant with temperature.

Also, pet peeve, there is nothing called ”degrees Kelvin”. The unit of temperature is just ”Kelvin”, nothing else.
 
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FAS1998 said:
I believe c(x,u) gives the energy per unit mass required to raise the temperature by 1 degree Kelvin as a function in of position and temperature.
When c varies with temperature, it is better to define it by saying that c(x,u)du is the energy required per unit mass to raise the temperature from u to u+du. Now the value of c is different, because the temperature is different. To increase temperature by another du requires heat c(x, u+du)du. Adding these steps together, from the initial to the final temperature, gives the integral you require. (I think you meant to say int(0→u), not int(u→u))
You cannot simply multiply c by the temperature interval u when c varies with temperature.
 
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Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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