Modes of
transmission
There are three distinct methods by which heat can be
transferred or propagated: (1) conduction, (2) convection and (3) radiation.
Conduction is the mode of transmission of heat in which heat
energy travels from one particle to another in the direction of decreasing
temperature without any bodily movement of the material particles from their
normal positions. Maxwell defined it as “the
flow of heat through an unequally heated body from places of higher to places of
lower temperature.” The power of transmitting heat in this way is possessed
by all substances, solids, liquids and gases, to a varying degree.
Convection |
Convection is the mode of heat transference in which the
material particles conveying the heat are carried from one place to another
place until the whole mass of the substance becomes uniformly heated. Maxwell
defined it as “the motion of the hot body
itself carrying its heat with it.” The power of transmitting heat in this
manner by the actual motion of the heated particles is possessed by liquids and
gases.
Thus the transference of heat either by conduction or
convection requires essentially a material medium (intervening medium).
But there is yet another mode of transference of heat
in which no material medium is needed. We get heat from the sun on earth,
although there is no continuous material medium between the sun and the earth.
This mode of transmission of heat is called radiation.
Radiation is that mode of transmission
of heat in which heat energy travels from the source of heat to its recipient
without any material medium taking part in it. Maxwell defined it as follows: “In radiation, the hotter body loses heat and
the colder body receives heat by means of a process occurring in some
intervening medium which does not it self thereby become hot.” The
processes of conduction and convection are necessarily slow processes due to
the action of the intervening medium, while radiation travels with the enormous
velocity of light, that is, with 3x10¹ยบ cm./sec.
The present chapter deals with conduction and
convection and radiation is discusses in the last chapter.
Conduction
According to the kinetic theory, the ultimate
particles or molecules of a body are in a state of incessant motion to and fro.
When a body is heated, the molecules there vibrate more vigorously and this
increased agitation (i.e. the increased heat energy) is passed on by collision
from particle to particle. Consider the mechanism
of conduction of heat to the other end of a metal bar heated at one end. Here
heat is first communicated to particles of the bar in contact with source of
heat. These particles, as a result, vibrate more vigorously about their respective
mean positions of rest and transfer the energy to adjacent particles by
collision; and these in their turn to the next layer of particles and so on.
The energy of vibration so transferred from layer to layer is nothing but the
heat transferred by conduction. Some substances conduct heat better than
others. There is an approximate rule that good electrical conductors are also
good thermal conductors and so metals are generally good conductors, while
substances like glass, mica, ebonite, felt, etc. are all bad conductors. Air
and other gases are bad conductors of heat. The good thermal conductivity of
metals has been partly ascribed to the presence of free electrons in them. The
free electrons behave as mobile molecules of a perfect gas and as such help in
the rapid transference of heat from one part of the metal to the other.
Convection
Convection molecule |
If a hot piece of metal is suspended in air, the air
immediately around it is heated by conduction and radiation. This causes an
expansion and a decrease in density so that air rises and cold air flows in
from below and from the sides to take its place. This continuous until the
metal is cooled to room temperature. Such air movement is termed natural convection. If a streaming is
maintained by some external agency, such as a fan or a pump, the process is
called forced convection.
As detailed study of the phenomenon of convection is
beyond the scope of this book, we shall illustrate here only some of its
practical applications in science and technology and some natural phenomena
where convection plays an important role.
Application
in science:
Newton’s law of
cooling
When a liquid is cooled by a drought of air, the rate
of loss of heat is proportional to the difference between the temperature the
liquid and that of the surroundings.
Natural
phenomena:
Winds
Winds are caused by convection currents set up in the
atmosphere as a result of unequal heating of the earth by the sun.
Land and
sea breezes
Convection currents account for land and sea breezes.
Sea breeze
Land having a lower a specific heat and a greater
absorbing power than water becomes more heated than the sea by the sun’s heat
during the day time. Consequently in the evening the air above the land becomes
more heated and rises up and cooler air from the sea blows towards the land to
take its place by convection, causing what is known sea breeze.
Land breeze
Since good absorbers are good radiators, during the
night the land loses more heat than the sea. On account of its lower specific
heat, the temperature of the land will become lower than that of the sea in the
early hours of the morning. As a result, the air above the land becomes cooler
than that above the sea. So colder air from over the land blows towards the sea
by convection causing what is called the land
breeze.
Trade winds
The earth in the tropics becomes more heated and this
heat is communicated to the air which is consequently heated. This heated air
being lighter rises up and to replace this colder air from the north and the
south flows towards the equator, but owing to the rotation of the earth from
west to east, the wind gets a resulting velocity in the north-eastern direction
in the northern hemisphere and south-eastern direction in the southern
hemisphere. The first is known as the north-east
trade wind and the other as the south-east
trade wind.
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