Heat flow through rubber sample

Click For Summary

Discussion Overview

The discussion revolves around the heat flow through a rubber sample subjected to a temperature gradient. Participants explore the time it would take for the center of the rubber sample to reach a specified temperature when exposed to a higher temperature on all surfaces. The conversation includes theoretical considerations of heat conduction, transient heat transfer, and the applicability of equations in different geometrical contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a rubber sample with specific dimensions and thermal properties, seeking guidance on the time required for the center to reach a target temperature.
  • Another participant asserts that the temperature will never fully reach the target but will get very close, prompting requests for clarification on this claim.
  • Discussion includes the concept of asymptotic behavior in transient heat conduction, with references to thermal diffusivity and a specific equation relating to the time to approach steady state.
  • Some participants question the validity of the assertion that equilibrium cannot be reached in finite time, arguing that thermal equilibrium is observable in practice.
  • There are inquiries about the applicability of the derived equations to larger or different geometrical configurations, such as hollow cylinders, and whether 2D considerations are necessary.
  • Participants express differing views on the implications of the heat equation and its assumptions, particularly regarding the discrete nature of materials and practical observations of thermal equilibrium.

Areas of Agreement / Disagreement

Participants do not reach consensus on whether the rubber sample can achieve thermal equilibrium in finite time. Some argue it will approach the target temperature asymptotically, while others contend that practical observations indicate equilibrium is reached. The applicability of equations to different geometries also remains a point of contention.

Contextual Notes

Limitations include assumptions about the material properties, the simplifications made in the heat conduction equations, and the potential neglect of heat loss in certain geometrical configurations.

examorph
Messages
39
Reaction score
0
I have a rubber sample here, basically it is a slice with a diameter of 45mm and a depth of 3mm. If this sample was at 25 degrees Celsius and I applied 180 degrees temperature all around it (top, bottom faces and outside diameter) how long would it take for the centre point (last point to get heated) to reach the 180 degrees Celsius temperature?

The materials thermal properties are:

Thermal Conductivity: 0.36 W/m*K
Specific Heat Capacity: 2 kJ/Kg K

I am really stuck with this and would appreciate any guidance at all. Thank you.
 
Science news on Phys.org
It will never happen - but it will get very, very close.
 
Thank you for the reply, could you please explain why it would never happen and also how long would it take to get very close?
 
Scott is right. It will approach 180 asymptotically. However, on a practical basis, it will approach 180 very closely in a finite amount of time. This is a transient heat conduction problem to a slab. The half-thickness of the slab is b=0.15 cm, and the thermal diffusivity of the rubber (based on the data you provided and a density of 1 gm/cc) is about α=0.0018 cm2/sec. The center of the slab should closely approach steady state when

\frac{αt}{b^2}=1.2

I leave it to you to calculate t.

Chet
 
Thank you very much, the results were similar to what I got from my simulations also. Could you please help me understand what this equation is?
I searched for it online and kept on running into the energy equation: https://imageshack.com/i/0k6mvlp
Is this where the equation came from and if so, it looks very familiar, it reminds me of the Navier-Stokes equation used in fluid dynamics, does it have a similar derivation?

Also, could you explain how you got the value 1.2 to me please.
 
examorph said:
Thank you very much, the results were similar to what I got from my simulations also. Could you please help me understand what this equation is?
I searched for it online and kept on running into the energy equation: https://imageshack.com/i/0k6mvlp
Is this where the equation came from and if so, it looks very familiar, it reminds me of the Navier-Stokes equation used in fluid dynamics, does it have a similar derivation?

Also, could you explain how you got the value 1.2 to me please.

See Transport Phenomena by Bird, Stewart, and Lightfoot. There is a chapter on Temperature Variations with More Than One Independent Variables. In the equation you showed, the velocity is equal to zero, and the heat generation rate is equal to zero. This gives the 1D transient heat conduction equation. Bird et al presents a set of 3 graphs showing transient temperature profiles for a slab, a cylinder, and a sphere. In the graph for a slab, a Fourier number of 1.2 looked like it would be about adequate for the center temperature to approach the wall temperature.

chet
 
Thank you very much for your help, it is greatly appreciated!

When I start looking at thicker, larger cross section 1D problems will I need to use different equations or would the above equation still apply?

Also, if I have a large diameter hollow cylinder such as that shown below, with a temperature applied to the top face could I apply the 1D formula on the 2D cross section (slice) of the cylinder to determine how long it would take for the heat to transfer??
http://www.onlinemathlearning.com/image-files/surfaceareahollowcylinder.gif
 
examorph said:
Thank you very much for your help, it is greatly appreciated!

When I start looking at thicker, larger cross section 1D problems will I need to use different equations or would the above equation still apply?

The same equation would still apply.
Also, if I have a large diameter hollow cylinder such as that shown below, with a temperature applied to the top face could I apply the 1D formula on the 2D cross section (slice) of the cylinder to determine how long it would take for the heat to transfer??
http://www.onlinemathlearning.com/image-files/surfaceareahollowcylinder.gif

The same equation would apply if the cylindrical surfaces are insulated, or the cylinder is very short. Otherwise, there can be heat loss out the sides.
 
.Scott said:
It will never happen - but it will get very, very close.
This is ridiculous.

The entire sample of rubber will reach thermal equilibirum in a finite time. That's an observable fact. If you have an equation that says otherwise, either that equation is wrong or an approximation to reality.
 
  • #10
Thanks for the replies, what if I was trying to find out how long it would take a cylinder such as that shown in my pervious post to reach the wall temperature. The conditions are that there would be a temperature applied to the outside diameter surface, inside diameter surface and top/bottom. Would this now become a 2D problem and require a 2D version of the energy transportation equation? If so, could you please give me an example?
Also, I would imagine that something bigger than a slab would not reach equilibrium in a finite time therefore, the results should be similar to what occurs in reality, is this true?
 
  • #11
examorph said:
Thanks for the replies, what if I was trying to find out how long it would take a cylinder such as that shown in my pervious post to reach the wall temperature. The conditions are that there would be a temperature applied to the outside diameter surface, inside diameter surface and top/bottom. Would this now become a 2D problem and require a 2D version of the energy transportation equation? If so, could you please give me an example?

If the annular thickness is small compared to the cylinder diameter, then you can neglect the curvature, and the result will still be the same as a flat slab. You can also neglect the 2D feature if you are willing to accept the infinitely-wide slab result as an upper bound to the true amount of time required for the annulus.
Also, I would imagine that something bigger than a slab would not reach equilibrium in a finite time therefore, the results should be similar to what occurs in reality, is this true?
I don't understand this question.

Chet
 
  • #12
DrClaude said:
This is ridiculous.

The entire sample of rubber will reach thermal equilibirum in a finite time. That's an observable fact. If you have an equation that says otherwise, either that equation is wrong or an approximation to reality.

If it reaches equilibrium in a finite amount of time, please tell us exactly what your equation for that finite amount of time is (in terms of the thickness of the slab and the physical properties of the material). Also tell us how you determine observationally the precise finite moment that equilibrium has been reached.

Chet
 
Last edited:
  • Like
Likes   Reactions: 1 person
  • #13
Chestermiller said:
If it reaches equilibrium in a finite amount of time, please tell us exactly what your equation for that finite amount of time is (in terms of the thickness of the slab and the physical properties of the material). Also tell us how you determine observationally the precise finite moment that equilibrium has been reached.

Chet
I never said that I had an equation. I just found the statement "it will never happen" to be completely unhelpful, and actually wrong, as thermal equilibirum is reached in practice.

The heat equation might say that equilibrium is only reached asymptotically, but the model neglects both the discrete (molecular) nature of the substance and the fact that the temperature of the environment need only be reached within the range of fluctuation of said temperature (or within the precision of the thermometer in the real world).

Just to be clear, I am not criticising the usefulness of the heat equation, just the usefulness of short, unhelpful answers that pop up on PF from time to time.
 
  • #14
DrClaude said:
I never said that I had an equation. I just found the statement "it will never happen" to be completely unhelpful, and actually wrong, as thermal equilibirum is reached in practice.

The heat equation might say that equilibrium is only reached asymptotically, but the model neglects both the discrete (molecular) nature of the substance and the fact that the temperature of the environment need only be reached within the range of fluctuation of said temperature (or within the precision of the thermometer in the real world).

Just to be clear, I am not criticising the usefulness of the heat equation, just the usefulness of short, unhelpful answers that pop up on PF from time to time.

Thanks DrClaude. I can certainly see what you are driving at. I was just a little concerned that your earlier response might possibly have detracted a bit (for the uninitiated) from the validity of the practical result I presented for calculating the time at which the sample effectively reaches equilibrium. On second thought, probably not.

Chet
 
  • #15
Thank you again for your help.

Is there some sort of rough ratio which I could use to determine whether or not the component that I am dealing can be considered as a flat slab or not?

For example I am currently dealing with a component which has an outer diameter of 120mm a width of 5mm (therefore a 110mm inner diameter) and a thickness of 10mm. Another component I am looking at has an outer diameter of about 300mm with all other dimensions being the same as above. Would the 1D energy transportation formula you described still apply?
 
  • #16
examorph said:
Thank you again for your help.

Is there some sort of rough ratio which I could use to determine whether or not the component that I am dealing can be considered as a flat slab or not?

Nominally, about 10:1.

For example I am currently dealing with a component which has an outer diameter of 120mm a width of 5mm (therefore a 110mm inner diameter) and a thickness of 10mm.
Actually, I think you mean that the thickness is 5 mm.
Another component I am looking at has an outer diameter of about 300mm with all other dimensions being the same as above. Would the 1D energy transportation formula you described still apply?

Actually, in my judgement, the 1D approximation would be adequate in both these cases.

chet
 
  • Like
Likes   Reactions: 1 person
  • #17
Thank you for all of the wonderful help it has really helped allot!

There is one thing that is still confusing me however. How is this equation independent of the temperature difference and contact area as I thought that these two variables played a large role in how heat traveled through a component?
 
  • #18
examorph said:
Thank you for all of the wonderful help it has really helped allot!

There is one thing that is still confusing me however. How is this equation independent of the temperature difference and contact area as I thought that these two variables played a large role in how heat traveled through a component?
The equation tells you when the temperature is reduced to a certain small fraction of the original temperature difference. So it's a percentage thing. The contact area determines the total amount of heat transferred, but this analysis focuses on the heat flow per unit area.

Chet
 
  • #19
So, based on this equation higher temperatures at the surface don't result in heat traveling faster through the component but rather the same distance when compared to a lower applied temperature but in larger quantities?

Also, you mentioned that a rough ratio of 10:1 could be used to determine whether or not to use the 1D equation,if this ratio was not met would I have to move onto the 2D equation? Is there any other cases in which I would have to leave the 1D equation and instead use 2D? Also, does the 2D equation also compare the temperature difference as a percentage?

Thank you.
 
  • #20
examorph said:
So, based on this equation higher temperatures at the surface don't result in heat traveling faster through the component but rather the same distance when compared to a lower applied temperature but in larger quantities?

yes
Also, you mentioned that a rough ratio of 10:1 could be used to determine whether or not to use the 1D equation,if this ratio was not met would I have to move onto the 2D equation?
No. it's still 1D radial, but the more exact solution involves the ratio of the diameters. The two solutions merge when the ratio of the diameter to the thickness becomes large. You can probably find the solution in Carslaw and Jaeger, Conduction of Heat in Solids.
Also, does the more exact equation also compare the temperature difference as a percentage?

It gives the absolute temperature difference as a direct proportion to the initial temperature difference. You can divide both sides of the equation by the initial temperature difference to get the percentage, which is independent of the initial temperature difference.

Chet
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 9 ·
Replies
9
Views
4K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 25 ·
Replies
25
Views
5K
  • · Replies 23 ·
Replies
23
Views
2K