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Temperature Regulation of the
Human Body
1
• The human body has the remarkable
capacity for regulating its core
temperature somewhere between
98°F and 100°F when the ambient
temperature is between
approximately 68°F and 130°F
2
• The external heat transfer mechanisms
are radiation, conduction and
convection and evaporation of
perspiration. The process is far more
than the passive operation of these heat
transfer mechanisms, however. The body
takes a very active role in temperature
regulation.
3
Heat Radiation
• Thermal radiation is energy transfer by the
emission of electromagnetic waves which
carry energy away from the emitting object.
For ordinary temperatures (less than “red
hot”), the radiation is in the infrared region of
the electromagnetic sprectrum.
4
• The relationship governing the net radiation
from hot objects is called the Stefan-
Boltzmann law:
5
Heat Conduction
• Conduction is heat transfer by means of
molecular agitation within a material without any
motion of the material as a whole. If one end of a
metal rod is at a higher temperature, then energy
will be transferred down the rod toward the
colder end because the higher speed particles
will collide with the slower ones with a net
transfer of energy to the slower ones. For heat
transfer between two plane surfaces, such as
heat loss through the wall of a house, the rate of
conduction heat transfer is:
6
= heat transferred in time = t
= thermal conductivity of the barrier
area
= temperature
= thickness of barrier
7
Thermal Conductivity
• Heat transfer by conduction involves transfer
of energy within a material without any
motion of the material as a whole. The rate of
heat transfer depends upon the
temperature gradient and the thermal
conductivity of the material.
• Conceptually, the thermal conductivity can be
thought of as the container for the medium-
dependent properties which relate the rate of
heat loss per unit area to the rate of change of
temperature.
8
9
Heat Convection
• Convection is heat transfer by mass motion of
a fluid such as air or water when the heated
fluid is caused to move away from the source
of heat, carrying energy with it. Convection
above a hot surface occurs because hot air
expands, becomes less dense, and rises. Hot
water is likewise less dense than cold water
and rises, causing convection currents which
transport energy.
10
11
Convection can also lead to
circulation in a liquid, as in
the heating of a pot of
water over a flame. Heated
water expands and
becomes more buoyant.
Cooler, more dense water
near the surface descends
and patterns of circulation
can be formed, though they
will not be as regular as
suggested in the drawing.
12
Convection cells are visible in
the heated cooking oil in the
pot at left. Heating the oil
produces changes in the index
of refraction of the oil, making
the cell boundaries visible.
Circulation patterns form, and
presumably the wall-like
structures visible are the
boundaries between the
circulation patterns.
13
Perspiration Cooling of Body
When the ambient temperature is
above body temperature, then
radiation, conduction and
convection all transfer heat into the
body rather than out. Since there
must be a net outward heat transfer,
the only mechanisms left under those
conditions are the evaporation of
perspiration from the skin and the
evaporative cooling from exhaled
moisture. Even when one is unaware
of perspiration, physiology texts quote
an amount of about 600 grams per
day of "insensate loss" of moisture
from the skin.
14
• The cooling effect of perspiration evaporation
makes use of the very large heat of
vaporization of water. This heat of
vaporization is 540 calories/gm at the boiling
point, but is even larger, 580 cal/gm, at the
normal skin temperature.
• As part of the physiological regulation of body
temperature, the skin will begin to sweat
almost precisely at 37°C and the perspiration
will increase rapidly with increasing skin
temperature.
15
Heat Transfer by Vaporization
• If part of a liquid evaporates, it cools the liquid
remaining behind because it must extract the
necessary heat of vaporization from that
liquid in order to make the phase change to
the gaseous state. It is therefore an important
means of heat transfer in certain
circumstances, such as the cooling of the
human body when it is subjected to ambient
temperatures above the normal body
temperature.
16
Cooling by Evaporation
• Because of the large heat of vaporization of
water, the evaporation from a liquid surface is
a very effective cooling mechanism. The
human body makes use of evaporative cooling
by perspiration to give off energy even when
surrounded by a temperature higher than
body temperature. The cooling process is an
example of the approach to thermal
equilibrium.
17
The evaporative cooling rate is given by
The cooling rate for a liquid (below
boiling) is more complicated since the
heat of vaporization changes with
temperature, and the rate of evaporation
depends upon ambient temperature
and relative humidity.
18

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Temperature Regulation Of The Human Body

  • 1. Temperature Regulation of the Human Body 1
  • 2. • The human body has the remarkable capacity for regulating its core temperature somewhere between 98°F and 100°F when the ambient temperature is between approximately 68°F and 130°F 2
  • 3. • The external heat transfer mechanisms are radiation, conduction and convection and evaporation of perspiration. The process is far more than the passive operation of these heat transfer mechanisms, however. The body takes a very active role in temperature regulation. 3
  • 4. Heat Radiation • Thermal radiation is energy transfer by the emission of electromagnetic waves which carry energy away from the emitting object. For ordinary temperatures (less than “red hot”), the radiation is in the infrared region of the electromagnetic sprectrum. 4
  • 5. • The relationship governing the net radiation from hot objects is called the Stefan- Boltzmann law: 5
  • 6. Heat Conduction • Conduction is heat transfer by means of molecular agitation within a material without any motion of the material as a whole. If one end of a metal rod is at a higher temperature, then energy will be transferred down the rod toward the colder end because the higher speed particles will collide with the slower ones with a net transfer of energy to the slower ones. For heat transfer between two plane surfaces, such as heat loss through the wall of a house, the rate of conduction heat transfer is: 6
  • 7. = heat transferred in time = t = thermal conductivity of the barrier area = temperature = thickness of barrier 7
  • 8. Thermal Conductivity • Heat transfer by conduction involves transfer of energy within a material without any motion of the material as a whole. The rate of heat transfer depends upon the temperature gradient and the thermal conductivity of the material. • Conceptually, the thermal conductivity can be thought of as the container for the medium- dependent properties which relate the rate of heat loss per unit area to the rate of change of temperature. 8
  • 9. 9
  • 10. Heat Convection • Convection is heat transfer by mass motion of a fluid such as air or water when the heated fluid is caused to move away from the source of heat, carrying energy with it. Convection above a hot surface occurs because hot air expands, becomes less dense, and rises. Hot water is likewise less dense than cold water and rises, causing convection currents which transport energy. 10
  • 11. 11
  • 12. Convection can also lead to circulation in a liquid, as in the heating of a pot of water over a flame. Heated water expands and becomes more buoyant. Cooler, more dense water near the surface descends and patterns of circulation can be formed, though they will not be as regular as suggested in the drawing. 12
  • 13. Convection cells are visible in the heated cooking oil in the pot at left. Heating the oil produces changes in the index of refraction of the oil, making the cell boundaries visible. Circulation patterns form, and presumably the wall-like structures visible are the boundaries between the circulation patterns. 13
  • 14. Perspiration Cooling of Body When the ambient temperature is above body temperature, then radiation, conduction and convection all transfer heat into the body rather than out. Since there must be a net outward heat transfer, the only mechanisms left under those conditions are the evaporation of perspiration from the skin and the evaporative cooling from exhaled moisture. Even when one is unaware of perspiration, physiology texts quote an amount of about 600 grams per day of "insensate loss" of moisture from the skin. 14
  • 15. • The cooling effect of perspiration evaporation makes use of the very large heat of vaporization of water. This heat of vaporization is 540 calories/gm at the boiling point, but is even larger, 580 cal/gm, at the normal skin temperature. • As part of the physiological regulation of body temperature, the skin will begin to sweat almost precisely at 37°C and the perspiration will increase rapidly with increasing skin temperature. 15
  • 16. Heat Transfer by Vaporization • If part of a liquid evaporates, it cools the liquid remaining behind because it must extract the necessary heat of vaporization from that liquid in order to make the phase change to the gaseous state. It is therefore an important means of heat transfer in certain circumstances, such as the cooling of the human body when it is subjected to ambient temperatures above the normal body temperature. 16
  • 17. Cooling by Evaporation • Because of the large heat of vaporization of water, the evaporation from a liquid surface is a very effective cooling mechanism. The human body makes use of evaporative cooling by perspiration to give off energy even when surrounded by a temperature higher than body temperature. The cooling process is an example of the approach to thermal equilibrium. 17
  • 18. The evaporative cooling rate is given by The cooling rate for a liquid (below boiling) is more complicated since the heat of vaporization changes with temperature, and the rate of evaporation depends upon ambient temperature and relative humidity. 18