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The "radiation effect" results from [[Heat transfer#Radiation|radiation heat exchange]] between human bodies and surrounding surfaces, such as walls and ceilings.<ref name="Cengel">Çengel, Yunus A., Afshin J. Ghajar, and Mehmet Kanoglu. Heat and Mass Transfer Fundamentals and Applications. New York: McGraw Hill Higher Education, 2011. Print.</ref> It may lead to phenomena such as houses feeling cooler in the winter and warmer in the summer at the same temperature. For example, in a room in which air temperature is maintained at 22&nbsp;°C at all times, but in which the inner surfaces of the house is estimated to be an average temperature of 10&nbsp;°C in the winter or 25&nbsp;°C in the summer, heat transfer from the surfaces to the individual will occur, resulting in a difference in the perceived temperature.
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We can observe and compare the rate of radiation heat transfer between a person and the surrounding surfaces if we first make a few simplifying assumptions:
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* The heat exchange in the environment is in a "steady state", meaning that there is a constant flow of heat either into or out of the house.
The '''effect of radiation on perceived temperature''' explains many phenomena, including why houses feel colder in the winter and warmer in the summer, even though the thermostat reads exactly the same in both situations. This is due to a “radiation effect” which results from [[Heat transfer#Radiation|radiation heat exchange]] between our bodies and the surrounding surfaces of the walls and the ceiling.<ref name="Cengel">Çengel, Yunus A., Afshin J. Ghajar, and Mehmet Kanoglu. Heat and Mass Transfer Fundamentals and Applications. New York: McGraw Hill Higher Education, 2011. Print.</ref>

For example, take a room which is maintained at 22° Celsius at all times. The inner surfaces of the walls, floors, and ceiling of the house are estimated to be an average temperature of 10° Celsius in the winter, but in the summer they are 25° Celsius. We can compare the rate of radiation heat transfer between a person and the surrounding surfaces if we first make a few simplifying assumptions:
* The heat exchange in the environment is in a “steady state”, meaning that there is a constant flow of heat either into or out of the house.
* The person is completely surrounded by the interior surfaces of the room.
* The person is completely surrounded by the interior surfaces of the room.
* Heat transfer by convection is not considered.
* Heat transfer by convection is not considered.
* The walls, ceiling, and floor are all at the same temperature.
* The walls, ceiling, and floor are all at the same temperature.
For an average person, the outer surface area is 1.4 m², the surface temperature is 30° Celsius, and the emissivity (ε) is 0.95. Emissivity is the ability of a surface to emit radiant energy compared to that of a black body at the same temperature.<ref>"Emissivity: Definition and Influence in Non-contact Temperature Measurement." / 13.04.2013. N.p., n.d. Web. 12 Apr. 2013.</ref>
For an average person, the outer surface area is 1.4 m<sup>2</sup>, the surface temperature is 30&nbsp;°C, and the emissivity (ε) is 0.95. Emissivity is the ability of a surface to emit radiative energy compared to that of a black body at the same temperature.<ref>"Emissivity: Definition and Influence in Non-contact Temperature Measurement." / 13.04.2013. N.p., n.d. Web. 12 Apr. 2013.</ref>
We will be using the following equation to find out how much heat is lost by a person standing same room in summertime as compared to the winter, at exactly the same thermostat reading temperature:
We will be using the following equation to find out how much heat is lost by a person standing in the same room in summertime as compared to the winter, at exactly the same thermostat reading temperature:
:<math>\dot{Q}=\varepsilon\sigma A_s (T_s^4 - T_{surr}^4)</math>
Q ̇=εσA_s (T_s^4-T_surr^4)
Where Q ̇ is the rate of heat loss (W), ε is the emissivity of a person, σ is the [[Stefan-Boltzmann constant]] (5.670x〖10^(-8 )W/m2∙K4), As is the surface area of a person, Ts is the surface temperature of a person (K), and Tsurr is the surface temperature of the walls, ceiling, and floor (K). Please note that this equation is only valid for an object standing in a completely enclosed room, box, etc. <ref name=Cengel/>
Where <math>\dot{Q}</math> is the rate of heat loss (W), <math>\varepsilon</math> is the emissivity (or the ability of an objects surface to emit energy by radiation) of a person, <math>\sigma</math> is the [[Stefan–Boltzmann constant]] (<math>\sigma=5.670373 \times 10^{-8}\, \mathrm{W\, m^{-2}K^{-4}}</math>), <math>A_s</math> is the surface area of a person, <math>T_s</math> is the surface temperature of a person (K), and <math>T_{surr}</math> is the surface temperature of the walls, ceiling, and floor (K). This equation is only valid for an object standing in a completely enclosed room, box, etc.<ref name=Cengel/>


In the winter, the amount of heat loss from a person, when the inner surfaces of the room were 10 degrees Celsius, was found to be 152 Watts.
In the winter, the amount of heat loss from a person is then 152 Watts if the inner surfaces of the room is, for example, 10 degrees Celsius.
(Q ̇=(0.95)(5.67x〖10^(-8) )(1.4)[(30+273)^4-(10+273)^4 ]=152) ̇
:<math>\dot{Q}=0.95 \times 5.670373 \times 10^{-8} \times 1.4 \times ((30+273.15)^4 - (10+273.15)^4) = 152.17</math>


In the summer, the amount of heat loss from a person, when the inner surfaces of the room were 25 degrees Celsius, was found to be 40.9 Watts.
In the summer, the amount of heat loss from a person, when the inner surfaces of the room were 25 degrees Celsius, was found to be 40.9 Watts.
(Q ̇=(0.95)(5.67x〖10^(-8) )(1.4)[(30+273)^4-(25+273)^4 ]=40.9) ̇
:<math>\dot{Q}=0.95 \times 5.670373 \times 10^{-8} \times 1.4 \times ((30+273.15)^4 - (25+273.15)^4) = 40.9</math>

Thermal radiation is the form of radiation emitted by bodies because of their temperature. <ref>Siegel, Robert, and John R. Howell. Thermal Radiation Heat Transfer. New York: Taylor & Francis, 2002. Print.</ref>
It differs from other forms of electromagnetic radiation such as [[x-rays]], [[gamma rays]], [[microwaves]], radio waves, and television rays that are not related to temperature. Scientists have found that all bodies at a temperature above absolute zero emit thermal radiation.<ref>"The University of British Columbia." Thermal Radiation. N.p., n.d. Web. 12 Apr. 2013.</ref> People are constantly radiating their heat, but at different rates. From these values, the rate of heat loss from a person is almost four times as large in the winter than in the summer, which explains the “chill” we feel in the winter even if the thermostat setting is kept the same.<ref name=Cengel/>
Thermal radiation emitted by all bodies above absolute zero (-273.15&nbsp;°C).<ref>Siegel, Robert, and John R. Howell. Thermal Radiation Heat Transfer. New York: Taylor & Francis, 2002. Print.</ref><ref>"The University of British Columbia." Thermal Radiation. N.p., n.d. Web. 12 Apr. 2013.</ref> It differs from other forms of electromagnetic radiation such as [[x-rays]], [[gamma rays]], [[microwaves]] that are not related to temperature. Therefore, people constantly radiate their body heat, but at different rates depending on body and surrounding temperatures. From these values, the rate of heat loss from a person is almost four times as large in the winter than in the summer, which explains the "chill" we feel in the winter even if the thermostat setting is kept the same.<ref name=Cengel/>


==References==
==References==
{{reflist}}
References list


Category:Heat transfer
[[Category:Heat transfer]]

Latest revision as of 05:44, 4 March 2024

The "radiation effect" results from radiation heat exchange between human bodies and surrounding surfaces, such as walls and ceilings.[1] It may lead to phenomena such as houses feeling cooler in the winter and warmer in the summer at the same temperature. For example, in a room in which air temperature is maintained at 22 °C at all times, but in which the inner surfaces of the house is estimated to be an average temperature of 10 °C in the winter or 25 °C in the summer, heat transfer from the surfaces to the individual will occur, resulting in a difference in the perceived temperature.

We can observe and compare the rate of radiation heat transfer between a person and the surrounding surfaces if we first make a few simplifying assumptions:

  • The heat exchange in the environment is in a "steady state", meaning that there is a constant flow of heat either into or out of the house.
  • The person is completely surrounded by the interior surfaces of the room.
  • Heat transfer by convection is not considered.
  • The walls, ceiling, and floor are all at the same temperature.

For an average person, the outer surface area is 1.4 m2, the surface temperature is 30 °C, and the emissivity (ε) is 0.95. Emissivity is the ability of a surface to emit radiative energy compared to that of a black body at the same temperature.[2] We will be using the following equation to find out how much heat is lost by a person standing in the same room in summertime as compared to the winter, at exactly the same thermostat reading temperature:

Where is the rate of heat loss (W), is the emissivity (or the ability of an objects surface to emit energy by radiation) of a person, is the Stefan–Boltzmann constant (), is the surface area of a person, is the surface temperature of a person (K), and is the surface temperature of the walls, ceiling, and floor (K). This equation is only valid for an object standing in a completely enclosed room, box, etc.[1]

In the winter, the amount of heat loss from a person is then 152 Watts if the inner surfaces of the room is, for example, 10 degrees Celsius.

In the summer, the amount of heat loss from a person, when the inner surfaces of the room were 25 degrees Celsius, was found to be 40.9 Watts.

Thermal radiation emitted by all bodies above absolute zero (-273.15 °C).[3][4] It differs from other forms of electromagnetic radiation such as x-rays, gamma rays, microwaves that are not related to temperature. Therefore, people constantly radiate their body heat, but at different rates depending on body and surrounding temperatures. From these values, the rate of heat loss from a person is almost four times as large in the winter than in the summer, which explains the "chill" we feel in the winter even if the thermostat setting is kept the same.[1]

References

[edit]
  1. ^ a b c Çengel, Yunus A., Afshin J. Ghajar, and Mehmet Kanoglu. Heat and Mass Transfer Fundamentals and Applications. New York: McGraw Hill Higher Education, 2011. Print.
  2. ^ "Emissivity: Definition and Influence in Non-contact Temperature Measurement." / 13.04.2013. N.p., n.d. Web. 12 Apr. 2013.
  3. ^ Siegel, Robert, and John R. Howell. Thermal Radiation Heat Transfer. New York: Taylor & Francis, 2002. Print.
  4. ^ "The University of British Columbia." Thermal Radiation. N.p., n.d. Web. 12 Apr. 2013.