How Can Space Be Cold in a Vacuum Despite Molecular Vibration?

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SUMMARY

The discussion centers on the phenomenon of heat transfer in a vacuum, specifically addressing how space can be cold despite the presence of thermal radiation. It is established that heat transfer occurs through radiation in a vacuum, as conduction and convection are absent. Space radiates like a black body at approximately 4 Kelvin, and human bodies radiate heat at about 500 watts, necessitating significant caloric intake to compensate for heat loss. The conversation also clarifies that while in space, individuals primarily lose heat through radiation, contrasting with the more efficient heat transfer mechanisms present in water or air.

PREREQUISITES
  • Understanding of thermal radiation and the Stefan-Boltzmann Law
  • Knowledge of heat transfer mechanisms: conduction, convection, and radiation
  • Familiarity with the concept of black body radiation
  • Basic principles of thermodynamics and temperature measurement
NEXT STEPS
  • Research the Stefan-Boltzmann Law and its applications in thermal physics
  • Explore the properties of black body radiation and its significance in astrophysics
  • Study the effects of vacuum on human physiology and heat loss
  • Investigate the differences in heat transfer in various environments, such as water and air
USEFUL FOR

Physicists, engineers, astronauts, and anyone interested in thermodynamics, space science, or the effects of vacuum on human bodies.

  • #31
DaveC426913 said:
Compared to maximum radiative cooling in a vacuum, the loss in Antarctica is low(er).
It is lower, but certainly not worthy of the "low" label it was given. Even "medium" would have been a poor characterization.

PS: When we can actually get quantitative comparisons for cheap, why resort to vague, qualitative descriptions?
 
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  • #32
Gokul43201 said:
PS: When we can actually get quantitative comparisons for cheap, why resort to vague, qualitative descriptions?
True, but considering the OP's knowledge of the subject, I think numbers don't tell the whole story and need some framing.

To some extent, 'low' could be treated as "a small component of the total cooling (i.e. in Antarctica)", whereas 'high' could considered "a large component of the total cooling (i.e. in space)."
 
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  • #33
Can we pose it as such?
Im standing in the storm at T=220K (naked :D) and there is a wind blowing at 20 m/s. The ambient pressure is 1atm and assume Earth atmosphere with air weight 0.029kg/mol .

Assume crossectional area of my body is 1m2, Cp (air capacity at 200K) = 1650 J/kg.K, Cp_body= 3500 J/kg.K . My skin has emissivity 0.7 (?) My initial body temperature is 310K . [we are concerned with conduction which should be negligible, convection which should be somewhat important and radiation] ? Is there anything which I did not consider before I embark?
 
  • #34
Now that I am thinking about it, is the wind actually relevant? The wind acts only to slow down the process of equilibriation between body and the air, by keeping theT gradient between the body and air by blowing off the near skin molecules of air that my body heated. The body, even in height wind, cannot cool bellow the ambient air temperature, right?
 
  • #35
sneez said:
Now that I am thinking about it, is the wind actually relevant? The wind acts only to slow down the process of equilibriation between body and the air, by keeping theT gradient between the body and air by blowing off the near skin molecules of air that my body heated. The body, even in height wind, cannot cool bellow the ambient air temperature, right?

You may want to spend a few minutes searching on "wind chill"
 
  • #36
I sure did, is it than reasonalbe to assume the windchill temperature rather than the air temperature in this example?
 
  • #37
Well, quick back of envelope results given convection heat loss is 1/2 of radiative loss in wind from http://www.drphysics.com/convection/convection.html,where 1/3 of heat loss is due to convection without wind condition.

I got something order of 1000 W , due to conduction, convectin, radiation. No condensation, evaporation, prespiration assumed.

It seem that somebody was very interested in the body heat loss in the year 1937 :)
JSTOR: http://www.jstor.org/view/00278424/ap000883/00a00090/0?frame=noframe&userID=89c65748@hamptonu.edu/01cce4405b00501cbca2a&dpi=3&config=jstor
 
  • #38
sneez said:
Now that I am thinking about it, is the wind actually relevant? The wind acts only to slow down the process of equilibriation between body and the air, by keeping theT gradient between the body and air by blowing off the near skin molecules of air that my body heated.
Stop and think about that for a sec - you've felt wind before, right? You've worn heavy clothes, right? The purpose of heavy clothes (insulation) is to create a shallow temperature gradient. With no clothes and a heavy wind, you have the steepest possible temperature gradient and since heat loss is proportional to that gradient, you have the maximum possible heat loss.

You have it exactly backwards.
The body, even in height wind, cannot cool bellow the ambient air temperature, right?
Of course. But that's the steady-state condition where you are frozen solid and in a normal winter, that takes hours. We're talking about the heat loss in the beginning, when your body temperature is near normal and you are not dead.
I sure did, is it than reasonalbe to assume the windchill temperature rather than the air temperature in this example?
I don't think that's Integral's point. The point is that "wind chill" is a measure of convective heat loss. It is basically how cold still air would have to be to provide the same convective heat loss as windy air at a higher temperature.
 
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  • #39
sneez said:
Well, quick back of envelope results given convection heat loss is 1/2 of radiative loss in wind from http://www.drphysics.com/convection/convection.html,where 1/3 of heat loss is due to convection without wind condition.
I'm not sure where you are getting the 1/2 number, and in the "other work" section, others who have calculated the ratio got .7 instead of 1/3 (2nd and fourth paragraphs). With wind, the first saw a 40% increase in convective rate with a 1mph wind (very, very low wind) and the fourth saw a 178% increase (10W/m^2) in a 3 m/s (2 mph) wind. So as that shows, the effect of wind is huge. With a very light wind (ie, just by walking), the convective heat loss rate swamps the radiative heat loss rate.

Note that these calculations are for room temperature air...
 
  • #40
thanx for the input russ

Stop and think about that for a sec - you've felt wind before, right? You've worn heavy clothes, right? The purpose of heavy clothes (insulation) is to create a shallow temperature gradient. With no clothes and a heavy wind, you have the steepest possible temperature gradient and since heat loss is proportional to that gradient, you have the maximum possible heat loss.

Thats exactly what I thought I said.

Of course. But that's the steady-state condition where you are frozen solid and in a normal winter, that takes hours. We're talking about the heat loss in the beginning, when your body temperature is near normal and you are not dead.

1st point:Are you implying that it is possible for anybody temperature to cool below the T of the air due to wind effects at certain conditions?

2nd: explain how that is not applicable in the beginning
I don't think that's Integral's point. The point is that "wind chill" is a measure of convective heat loss. It is basically how cold still air would have to be to provide the same convective heat loss as windy air at a higher temperature.
Thats exactly why I posed it as a question , do you have an answer? And due to its definition I think its reasonable to use the concept in the wind condition. Basically, I use wind chill temperature in calculation as a temperature surrounding air would "have" given no wind.

I'm not sure where you are getting the 1/2 number, and in the "other work" section, others who have calculated the ratio got .7 instead of 1/3 (2nd and fourth paragraphs). With wind, the first saw a 40% increase in convective rate with a 1mph wind (very, very low wind) and the fourth saw a 178% increase (10W/m^2) in a 3 m/s (2 mph) wind. So as that shows, the effect of wind is huge. With a very light wind (ie, just by walking), the convective heat loss rate swamps the radiative heat loss rate.
I sort of arbitrarily assumed it. The article claims 1/3 and other sources also cite that, but that's for no wind condition, I thought with wind convection gets more and more important as you say, so I gave it more importance .
 
  • #41
sneez said:
Thats exactly what I thought I said.
You said the wind slows the body reaching equilibrium with the air - it speeds it up.
1st point:Are you implying that it is possible for anybody temperature to cool below the T of the air due to wind effects at certain conditions?
Certainly not.
2nd: explain how that is not applicable in the beginning
The body isn't frozen solid, so talking about how heat would be removed when it is frozen solid is irrelevant.
Thats exactly why I posed it as a question , do you have an answer?
?? An answer to what? If we should assume wind chill temp? I guess if your equation doesn't have a term for wind speed, you can use the wind chill temp instead.
 
  • #42
sneez said:
1st point:Are you implying that it is possible for anybody temperature to cool below the T of the air due to wind effects at certain conditions?
Yes! That is why we sweat. Otherwise everyone in Phoenix would die.

However, I think sweat would be a pretty small factor in Antartica :-)
 
  • #43
Right, speed up by faster heat removal, i stand corrected.

DaeSpam, sweat is cooling by evaporation, I was trying to see if object will cool below the air temperature just due to wind alone.

(I don't think I am understanding the russ's comment on the steady state of frozen solid)
 
  • #44
sneez said:
DaeSpam, sweat is cooling by evaporation, I was trying to see if object will cool below the air temperature just due to wind alone.
So neglecting evaporation just considering convection? No, I don't think that convection can cool things below the air temperature. I think the only way that would even be theoretically possible is for the the flow to cause some unusually low pressure region which would experience an adiabatic drop in temperature. But surely such effects would be negligably small and very difficult to model for a human. The wind-tunnel tests might be fun though!
 
  • #45
that depends on how you define heat. if you mean hot or warm for a human, then there is very little heat in the universe. if you mean above absolute zero, then most of the universe has heat.
 

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