Understanding the Stefan-Boltzmann Law (when the surroundings are hotter)

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SUMMARY

The discussion centers on the Stefan-Boltzmann Law, expressed as H = AσT^4, where H is the energy emitted per unit time, A is the object's area, and T is its absolute temperature. It clarifies that σ represents the Stefan-Boltzmann constant, while emissivity (ε) varies between 0 and 1 for real materials, with ε = 1 for black bodies. The relationship between the Stefan-Boltzmann Law, Newton's Law of Cooling, and conduction is established, indicating that the former can be applied in all cases of heat transfer, while the latter two are special cases for small temperature differences. The discussion emphasizes the importance of understanding heat flow direction and the distinction between radiation and conduction/convection.

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  • Understanding of the Stefan-Boltzmann Law and its formula H = AσT^4
  • Knowledge of emissivity and its relationship to the Stefan-Boltzmann constant
  • Familiarity with Newton's Law of Cooling and its application
  • Basic principles of heat transfer, including conduction and convection
NEXT STEPS
  • Study the derivation and applications of the Stefan-Boltzmann Law in thermal radiation
  • Explore the concept of emissivity and its impact on material heat transfer
  • Investigate the conditions under which Newton's Law of Cooling applies
  • Learn about the differences between conduction, convection, and radiation in heat transfer
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JC2000
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TL;DR
1.My book tells me that given ##T_{surroundings}##, and ##T## of the object radiating heat, the law is expressed as ##H = \sigma A (T^4 - T^4_{surroundings})##.

2. Relating Newton's Law of Cooling, Conduction, and Stefan-Boltzmann Law

3. Is emissivity the same as Stefan's constant or is it ## e * \sigma## where ##e## varies, depending on the material?
1.If so what would the law mean if ##T_{surroundings}>T##?

2. Stefan-Boltzmann Law is formulated as ##H = A\sigma T^4## where ##H## is the energy emitted per unit time, ##A## is the area of the object, ##T## is the absolute temperature of the object and (3.) I am unclear about whether ##\sigma## represents emissivity or ##e*\sigma## represents Stefan's constant.

My book also defines Conduction (as the time rate of heat flow for a given temperature difference), as ##H = kA \frac {T_c - T_d}{L}## where ##H## is the rate of flow of heat (heat current), ##A## is the area of cross-section and ##L## is the length between the two points being considered, ##T_c - T_d## the temperature difference between the points.

Newton's Law of Cooling is stated as a special case of Stefan-Boltzmann Law where the temperature difference is very small and is formulated as ##\frac {dQ}{dt} = k(T_2 - T_1)##.

I feel that the three must be somehow interrelated, am I correct in assuming this? If so, how?

3. Lastly is emissivity the same as Stefan's constant or is it ## e * \sigma## where ##e## varies, depending on the material?

Thank you!
 
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Hi JC
1. the object has a net absorption of radiation
2. e represents emissivity, σ represents the Stefan - Boltzmann constant
3. ε = 1 for a black body. For all real materials, it varies from 0 to 1, and can be frequency dependent.

Newton's Law of cooling - if the temperature difference is large, then radiation effects should be taken into account
 
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1. So ##H## represents the rate of absorption? (If so, shouldn't heat absorption have a positive sign and hence rate of heat absorption should also have a positive sign?)
2. Thanks that makes it clear!
3. So, it is safe to say that Stefan-Boltzmann's law could be used in place of the other two formulas while the other two are special cases (for small T differences we have Newton's Law of Cooling and the formula of conduction is when heat transfer is occurring within a substance). Thus Stefan-Boltzmann's law could be used to find the rate of heat transfer in all cases?
 
JC2000 said:
1. So ##H## represents the rate of absorption? (If so, shouldn't heat absorption have a positive sign and hence rate of heat absorption should also have a positive sign?)
2. Thanks that makes it clear!
3. So, it is safe to say that Stefan-Boltzmann's law could be used in place of the other two formulas while the other two are special cases (for small T differences we have Newton's Law of Cooling and the formula of conduction is when heat transfer is occurring within a substance). Thus Stefan-Boltzmann's law could be used to find the rate of heat transfer in all cases?
1. In which direction you assign heat flow, in or out, would be case dependent.
Example - the sun outputs X amount of radiation, so one would consider that a positive value for the sun.
the Earth receives Y amount of heat flux, so one would consider that as a positive value for the earth.

3. probably not. Conduction and convection are heat transfers by contact, not by radiation.
 
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