Newton's law of cooling of a surface

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Homework Help Overview

The discussion revolves around Newton's law of cooling, particularly its applicability under various conditions, such as when heat loss occurs through both convection and radiation. Participants explore scenarios where the law may not hold, questioning the impact of temperature uniformity and the nature of heat transfer mechanisms.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Some participants question the validity of Newton's law of cooling when surface and surrounding temperatures are not uniform. Others discuss the conditions under which the law applies, particularly in the presence of radiation alongside convection.

Discussion Status

The discussion is active, with participants offering various perspectives on the applicability of Newton's law of cooling. There is recognition of the differences between convection and radiation, and some participants are exploring how these mechanisms interact, particularly at small temperature differences.

Contextual Notes

Participants note the importance of the convection coefficient and its dependence on external conditions, as well as the potential confusion arising from the terminology used in discussing heat transfer mechanisms.

sachi
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I'm having trouble thinking of an instance when Newton's law of cooling is no longer valid. could it have something to do with the surface of the system or the surroundings not having uniform temperature.

thanks very much
 
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What do you mean by no longer valid? If you can expand on that just a bit it might make this a bit easierr. The only way there would be no heat transfer is if the surface temperature is equal to the surrounding temperature. Even if there wasn't an even distribution, it would still be valid. I guess the other way it could not be valid is if you had a non-real heat transfer coefficient, but I can not see how that would be physically possible.
 
sachi said:
I'm having trouble thinking of an instance when Newton's law of cooling is no longer valid. could it have something to do with the surface of the system or the surroundings not having uniform temperature.
thanks very much

A generalized version of the Newton law of cooling may be:

[tex]q(x,y,z,t)=h(x,y,z,t)(T(x,y,z,t)-T_\infty(x,y,z,t))[/tex]

The Newton law always hold, IF AND ONLY IF you calculate the convection coefficient h in a suitable way for your problem. In fact, one always is able to calculate h from this equation, by merely working it out. The value of the Newton law is relationed with experiments, because it is easy to calculate the heat flux based on experimental correlations, BUT this equation does NOT add any additional physical law to Navier-Stokes equations.
 
I think Newton's law of cooling is applicable without restriction to a body cooling by convection only.

So, in case a body of surface area [itex]A[/itex] at an absolute temperature [itex]T[/itex] is also losing heat by radiation, then Newton's law of cooling, ie, [tex]\frac{dT}{dt} = -bA(T-T_0)[/tex] will be valid only for small temperature differences between [itex]T[/itex] and [itex]T_0[/itex]. ([itex]T_0[/itex] is the temperature of surroundings which is less).

This will be because, by stefan's law, the net loss of energy due to radiation is
[tex]\Delta u = \sigma e A(T^4 -{T_0}^4)[/tex]

If the temperature difference is small,ie, [tex]T=T_0 + \Delta T[/tex] and [tex]T^4 -{T_0}^4[/tex] can be approximated as [tex]4{T_0}^3(T-T_0)[/tex].
So, the net rate of cooling in this case will also be [tex]\frac{dT}{dt} = -bA(T-T_0)[/tex]
 
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siddharth said:
I think Newton's law of cooling is applicable without restriction to a body cooling by convection only.

So, in case a body of surface area [itex]A[/itex] at an absolute temperature [itex]T[/itex] is also losing heat by radiation, then Newton's law of cooling, ie, [tex]\frac{dT}{dt} = -bA(T-T_0)[/tex] will be valid only for small temperature differences between [itex]T[/itex] and [itex]T_0[/itex]. ([itex]T_0[/itex] is the temperature of surroundings which is less).

This will be because, by stefan's law, the net loss of energy due to radiation is
[tex]\Delta u = \sigma e A(T^4 -{T_0}^4)[/tex]

If the temperature difference is small,ie, [tex]T=T_0 + \Delta T[/tex] and [tex]T^4 -{T_0}^4[/tex] can be approximated as [tex]4{T_0}^3(T-T_0)[/tex].
So, the net rate of cooling in this case will also be [tex]\frac{dT}{dt} = -bA(T-T_0)[/tex]

The What? I disagree completely with you. Radiation and Convection are two different mechanisms no matter how large is [tex]\Delta T[/tex]. The fact that radiation behaves in a similar fashion than convection when [tex]\Delta T[/tex] becomes small does NOT mean both things are the same. The convection coefficient has a STRONG dependence on the external flow, and has NOTHING to do with radiation, which is by the way relationed with the electronic structure of the solid.

A very wrong advice you gave this time.
 
Clausius2 said:
The What? I disagree completely with you. Radiation and Convection are two different mechanisms no matter how large is [tex]\Delta T[/tex]. The fact that radiation behaves in a similar fashion than convection when [tex]\Delta T[/tex] becomes small does NOT mean both things are the same. The convection coefficient has a STRONG dependence on the external flow, and has NOTHING to do with radiation, which is by the way relationed with the electronic structure of the solid.
A very wrong advice you gave this time.

I agree that convection and radiation are very different.

What I meant to say to the OP was that the formula for the net rate of cooling may not be applicable in when there is heat loss due to radiation also.

I think the confusion is because I used the words Newton's law of cooling while working with the case where heat is lost by radiation and convection.

What I meant was that the rate of fall of temperature due to radiation will also be [tex]bA(T-T_0)[/tex] when the temperature difference is small.

So the net rate of fall of temperature due to both radiation and convection will be [tex]\frac{dT}{dt} = -(b_1 + b_2)A(T-T_0)[/tex] and this formula is valid only when [tex]\Delta T[/tex] is small

Do you agree with what I am saying now?
 
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siddharth said:
I agree that convection and radiation are very different.

What I meant to say to the OP was that the formula for the net rate of cooling may not be applicable in when there is heat loss due to radiation also.

I think the confusion is because I used the words Newton's law of cooling while working with the case where heat is lost by radiation and convection.

What I meant was that the rate of fall of temperature due to radiation will also be [tex]bA(T-T_0)[/tex] when the temperature difference is small.

So the net rate of fall of temperature due to both radiation and convection will be [tex]\frac{dT}{dt} = -(b_1 + b_2)A(T-T_0)[/tex] and this formula is valid only when [tex]\Delta T[/tex] is small

Do you agree with what I am saying now?

If you mean that b1 and b2 are two different coefficients without any relation, and that Newton cooling law always hold despites there is radiation or not (ok, there is going to be some portion of q not taken into account due to radiation), then I am fine with your post.
 
Clausius2 said:
If you mean that b1 and b2 are two different coefficients without any relation, and that Newton cooling law always hold despites there is radiation or not (ok, there is going to be some portion of q not taken into account due to radiation), then I am fine with your post.

Yes, that's what I mean.
I probably should have made it clearer in my first post though.
 
Well, sorry, maybe I misunderstood your reply too. But to say the truth I remember one guy here who was convinced that at small [tex]\delta T[/tex] both things were the same. It was long time ago.
 

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