How does heat loss through conduction occur?

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SUMMARY

Heat loss through conduction is governed by the equation ΔQ = K*S*ΔT/D, where ΔQ represents energy flow, K is the material's thermal conductivity, S is the cross-sectional area, ΔT is the temperature difference, and D is the thickness of the material. The discussion highlights that while thicker insulation reduces heat flow, at thermal equilibrium, the thickness should not affect energy loss. However, during the transient state, temperature distribution varies over time and distance, as layers of material sequentially heat up. The mathematical modeling of one-dimensional heat conduction is essential for understanding these dynamics.

PREREQUISITES
  • Understanding of thermal conductivity and the concept of ΔQ in heat transfer.
  • Familiarity with the principles of steady-state and transient heat conduction.
  • Basic knowledge of mathematical modeling, particularly in one-dimensional heat conduction.
  • Awareness of temperature distribution concepts in materials over time.
NEXT STEPS
  • Study the mathematical modeling of one-dimensional heat conduction in detail.
  • Explore the concept of thermal resistance and its analogy to electrical resistance.
  • Investigate temperature distribution in transient heat conduction scenarios using simulation tools.
  • Review relevant literature on heat transfer principles, such as the resources provided in the discussion.
USEFUL FOR

Students and professionals in mechanical engineering, materials science, and thermal management, particularly those interested in heat transfer analysis and insulation design.

burashka5719
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Usually it is said that loss of heat through a chunk of material because of conduction is proportional to difference in temperature and inversely proportional to thickness of material.
E.g. if I got a wall to ΔQ = K*S*ΔT/D.
where ΔQ - is energy flow through material. K - constant characteristic to material , S - area through which energy flow happens, ΔT difference in temperature on both sides of material ( in direction of flow) and D - material thickness in direction of the flow.

What I don't understand, is why in case when the process has stabilised ( temperatures are constant on both side of material for a long time) D works to diminish the flow. I know that it is common sense, but I don't understand physics of this process. Can someone explain what happens it terms of atomic or molecular model?
Also, let's say we got a bar of homogenise material which is heated on one side. how looks distribution of temperature through a bar of material as function of time and distance from the point where heat is applied.
 
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burashka5719 said:
Also, let's say we got a bar of homogenise material which is heated on one side. how looks distribution of temperature through a bar of material as function of time and distance from the point where heat is applied.
At steady state, the graph of temperature from T1 to T2 through distance D is a straight line of constant slope.
 
256bits said:
At steady state, the graph of temperature from T1 to T2 through distance D is a straight line of constant slope.
Yes, but before the system stabilised? During this period distribution of temperature as function of time and distance from 0 can be different.
 
Think of the block as a series of layers stacked together . First layer has to heat up before it can heat next layer etc sequentially through the total thickness .

The layers don't just conduct heat they store it as well so it takes time for their temperatures to rise .

May be better to put this in mathematical form rather than descriptive . The mathematics for one dimensional heat conduction is relatively easy to understand .
 
Last edited:
burashka5719 said:
Yes, but before the system stabilised? During this period distribution of temperature as function of time and distance from 0 can be different.
Have a look at this Excel Animation. It shows the way the temperature varies in time over a 2D area when a hot object appears in it. It's a diffusion model.
 
Hello,
There are two questions in my original e-mail:
The second one - about temperature distribution as function of time and distance from heat source is more or less clear, but if someone can recommend where I can read about relevant math it would be great.
The first question actually is more of a problem: on one hand common sense tells that thicker insulation diminishes heat flow from high temperature area to cool area,
on the other hand, once the system reaches equilibrium ( constant temperature difference on both sides of insulator) it seams to me that insulator thickness shouldn't have any effect on amount of energy loss.
I try a very simplified model - a long bar of homogeneous material with constant cross section ( 1 dimensional problem) with constant temperature difference on both sides . Once equilibrium is reached insulator doesn't store heat anymore. So taking as example the above model - series of layers stacked together, why 10 or 1000 of layers will conduct less heat then a single one.
My feeling is that there is something that plays a role of resistance in electrical current transfer of flued transfer through a pipe, but in those cases there is energy loss through heat, which doesn't haven here,
 

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