What is the Relationship Between Heat Energy and Temperature?

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SUMMARY

The relationship between heat energy and temperature is defined by the equation e(x,t) = c(x)p(x)u(x,t), where e represents thermal energy per unit volume, c is specific heat, p is mass density, and u is temperature. The correct expression for the heat energy per unit mass necessary to raise the temperature from 0 to u(x,t) is given by the integral ∫₀ᵘ c(x,û) dû, rather than simply c(x)u(x,t). This integral accounts for variations in specific heat with respect to both position and temperature, confirming that c can be a function of x and u.

PREREQUISITES
  • Understanding of thermodynamics principles, specifically heat energy and temperature relationships.
  • Familiarity with calculus, particularly integration and the Fundamental Theorem of Calculus.
  • Knowledge of specific heat capacity and its dependence on temperature and position.
  • Basic concepts of mass density in relation to thermal energy.
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  • Study the Fundamental Theorem of Calculus in detail to understand its application in thermodynamics.
  • Research the implications of variable specific heat c(x,u) in thermal energy calculations.
  • Explore advanced topics in thermodynamics, focusing on heat transfer and energy conservation.
  • Practice solving problems involving integrals of functions dependent on multiple variables, particularly in physical contexts.
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Homework Statement



Show that the heat energy per unit mass necessary to raise the temperature of a thin slice of thickness \Deltax from 0^o{} to u(x,t) is not c(x)u(x,t). but instead \int_0^uc(x,\overline{u})d\overline{u}.

Homework Equations



According to the text, the relationship between thermal energy and temperature is given by

e(x,t) = c(x)p(x)u(x,t),

which states that the thermal energy per unit volume equals the thermal energy per unit mass per unit degree times the temperature time the mass density.

When the specific heat c(x) is independent of temperature, the heat energy per unit mass is just c(x)u(x,t).


The Attempt at a Solution



The only hint really is that this is related to the area, from the solution. How can I go about this geometrically and/or algebraically?

Any help/pointers will be much appreciated. Thank you!
 
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that integral doesn't make sense based on what you've posted, can you check it... c has changed to a function of x only or x and u (position and temperature)...?
 
Last edited:
so i think you do need to assume c = c(x,u), then try and find the change in energy de, for a small change in temp du and integrate.
 
Argh of course! Thank you very much! :approve:
 
I have used your advice and went about it in the following way:

For a small slice of thickness \Delta{x} a small change in energy will be given by

de = c(x,u)du

Dividing by du I obtain e_{u} = c(x,u).

From the Fundamental Theorem of Calculus, this really says that

e(x,t) = \int_0^uc(x,t)dt.

Am I correct in my thinking? It feels a bit messy somehow...
 
you can just start from differentials
de = c(x,u)du
\delta e = \int_{e_0}^{e_f}d\bar{e} = \int_{0}^{u} c(x,\bar{u})d\bar{u}
 
Your equation did not even occur to me but simplifies it a lot. Thank you very much for your help. I can now get some sleep again :-)
 

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