note on humidity
TRANSCRIPT
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HUMIDITY
HUMIDITY refers to the mass (lb. or kg) of water vapour per unit mass of dr air
or moles of water vapour per mole of dr air.
Humidit spe!ifs the amount of water vapor in the air.
Humidit is e"pressed in different was#
1. Absolute Humidity is the mass of water vapor in a given volume of air.
This is e"pressed as grams of water vapor in a !ubi! meter of air. (Is the per!entage
of water vapor a!tuall present in the air).
$"ample# if the water vapor in % !ubi! meter of air weighs &' grams the absolute
humidit of the air is &' grams!ubi! meters (&' gm&).
2. Specific humidity is the mass of water vapor !ompared with the mass of all the
air in the par!el (in!luding vapor).
3. Relative humidity is the absolute humidit divided b the amount of water that
could be present in the air. *elative humidit indi!ates the degree of !omfort or
dis!omfort one feels from the humidit be!ause it indi!ates the amount of
perspiration that !an evaporate from the skin.
4. The mixi! "#tio is the mass of water vapor divided b the mass of dr
air.
+oth spe!ifi! humidit and mi"ing ratio are e"pressed as grams of water
vapor per kilogram of air (gkg).
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De$ %oit&
The dew point is a good indi!ator of the air,s water vapor !ontent. High dew points
indi!ate high water vapor !ontent- !onversel low dew points indi!ate low water
vapor !ontent. ddition of water vapor to the air in!reases the dew point- removing
water vapor lowers it. This is the temperature at whi!h air attains saturation and a
further addition of water vapour whi!h leads to dew formation be!ause of
!ondensation of water vapour. It is rarel used to indi!ate the moisture !ontent of
airatmosphere.
Degree of /aturation#
It is stated as the ration of weight of water vapour in air at a given !onditions to the
weight of the water vappour in air at saturation keeping temperature !onstant. It is
also !alled saturation ratio or per!entage humidit.
Me#su"i! Humidity&
% ps!hrometer is an instrument used to determine the water vapor !ontent
of the air. It !onsists of two thermometers (dr bulb and wet bulb). fter
whirling the instrument the dew point and relative humidit !an be obtained
with the aid of the en!losed table.
0 hgrometer is an instrument designed to measure the air,s water vapor
!ontent. The sensing part of the instrument !an be hair (hair hgrometer) a
plate !oated with !arbon (ele!tri!al hgrometer) or an infrared sensor
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(infrared hgrometer). This instrument !an be used in the field and
greenhouse to measure both temperature and humidit.
%sych"omet"ic 'h#"t
1. It"oductio
The ps!hrometri! !hart shows graphi!all the parameters relating to water
moisture in air. This appli!ation note des!ribes the purpose and use of the
ps!hrometri! !hart
ir !omprises appro"imatel 123 nitrogen 0%3 o"gen and %3 other gases. +ut
air is never dr even in a desert. Two4thirds of the earth5s surfa!e is !overed with
water and this along with other surfa!e water and rain maintain low pressure
water vapor to be suspended in the air making up part of the %3 of other gases.
The ps!hrometri! !hart indi!ates the properties of this water vapor through the
following parameters ea!h of whi!h is e"plained in more detail below#
6 dr bulb temperature
6 wet bulb temperature (also known as saturation temperature)
6 dew point temperature
6 relative humidit
6 moisture !ontent (also known as humidit ratio)
6 enthalp (also known as total heat)
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6 spe!ifi! volume (the inverse of densit)
7or an e"ample on how the ps!hrometri! !hart is used in pra!ti!e please read
8ower 9not5s appli!ation note on measuring enthalp to evaluate the effi!ien! of
an air !onditioning sstem.
2. %"ope"ties o the 'h#"t
2.1 D"y bulb (D)* tempe"#tu"e
:e measure the temperature of the air with a thermometer. Traditional
thermometers have a bulb that !ontains a li;uid that e"pands and a tube indi!ating
the temperature on a s!ale. s the li;uid e"pands it rises up the s!ale.
:hi!hever method is used this measurement is !alled the dr bulb temperature
be!ause the end of the thermometer that is making the measurement has no
moisture on it.
The temperature of the air is measured in
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2.2 +et bulb (+)* tempe"#tu"e
The wet bulb temperature is measured b having the bulb
of the thermometer moist. The moisture evaporates lowering the temperature
re!orded b the thermometer. ?ess moisture in the air will result in a faster rate of
evaporation and therefore a !older reading. In pra!ti!e we !an use an ele!troni!
thermometer and wrap a paper tissue over the thermo!ouple. Make the paper tissue
moist but not too wet that water is dripping from it. Move air over the tissue (or
move the thermo!ouple through the air) so the water evaporates.
:hen the air sample is saturated with water (that is it has %@@3 relative
humidit) no water !an evaporate from the moist tissue so the :+ temperature
will read the same as the D+ temperature. This temperature is therefore also
referred to as the saturation temperature. This temperature is indi!ated b diagonal
lines on the !hart.
2.3 ,el#ti-e humidity (,H*
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This is the ratio of the fra!tion of water vapor in the air to
the fra!tion of saturated moist air at the same temperature and pressure. *H is
dimensionless and is usuall e"pressed as a per!entage. %@@3 *H indi!ates the air
is saturated and !annot hold an more moisture. 8referred values of !omfort for
people are between &'3 and A@3.
?ines of !onstant relative humidit are shown as e"ponential lines on the
ps!hrometri! !hart. The line at %@@3 is referred to as the saturation line.
2.4 De$ poit (D%* tempe"#tu"e
This is the temperature of the air at whi!h a moist air sample rea!hes water vapor
saturation. It is e;uivalent to a wet bulb temperature at %@@3 relative humidit. t
this !ombination of temperature and humidit further removal of heat results in
water vapor !ondensing into li;uid.
pra!ti!al view of the dew point is the temperature
to whi!h air must be !ooled before !ondensation will begin. n e"ample is when
ou take a bottle of beer out of the refrigerator. :ater !ondenses on the outside of
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the bottle onl if the original temperature of the bottle was below the dew point.
The instantaneous temperature of the water is the dew point temperature.
s a sample of air is !ooled its *H !limbs until it rea!hes %@@3 *H (saturated
air). This is the dew point temperature. t saturation the dew point temperature
e;uals the wet bulb temperature whi!h also e;uals the dr bulb temperature and
the *H is %@@3. This temperature is shown as hori>ontal lines on the !hart.
2. Moistu"e cotet
This is also known as the humidit ratio and is usuall designated as :. It is the
proportion of the mass of water vapor per unit mass of dr air. Humidit ratio is
dimensionless but in the U/ it is usuall e"pressed as pounds of moisture per
pound of dr air- elsewhere it ma be e"pressed as grams of water per kilogram of
dr air or as a per!entage.%
The moisture !ontent is the verti!al a"is of the !hart.
2./ 0th#lpy (tot#l he#t*
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$nthalp (usuall designated as h) is the total amount of
heat energ of the moist air and therefore in!ludes the amount of heat of the dr air
and the water vapor in the air. In the appro"imation of ideal gases lines of !onstant
enthalp are parallel to lines of !onstant :+ temperature. Thus the enthalp is
indi!ated b diagonal lines on the !hart.0
In the U/ enthalp is measured in +TU per pound of dr air- elsewhere it is
measured in Boules per kilogram of air.
2. Specific -olume
This is the inverse of densit. /pe!ifi! volume is therefore the volume per unit
mass of the air sample. This is shown as diagonal lines on the !hart.
In the U/ this is measured b !ubi! feet per pound of dr
air- elsewhere it is measured b !ubi! meters per kilogram of dr air.
2. 'omfo"t oes
8eople feel !omfortable within a small range of temperatures and humidities. The
ranges var based on where ou live and on the time of ear. In the northern
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hemisphere people tpi!all wear more !lothes in winter than in summer.
Therefore rooms are maintained at !ooler temperatures in winter than in summer.
8eople are sensitive to humidit be!ause water evaporates from the skin and this
evaporation !ools the bod. t a high humidit water evaporates from the skin
slowl so we feel warmer. t a low humidit water evaporates faster and we feel
!older. The effe!t of per!eived in!rease in temperature with in!rease in humidit is
referred to as the Heat Inde" and is shown graphi!all in the figure.%
This also e"plains wh some people in!rease the
temperature of a room after treating an air !onditioner with the /ntheti!
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*efrigeration =atalst. The treatment with the /ntheti! *efrigeration =atalst
makes the air !older. This !older air !ondenses more water moisture from the air
and lowers the humidit. 8eople !ompensate b raising the temperature and
thereb saving even more mone after treatment with the /ntheti! *efrigeration
=atalst.
The ps!hrometri! !hart shows the two !omfort >ones tpi!all a!!eptable for U/
!iti>ens.
3. 0x#mple uses of the psych"omet"ic ch#"t
4.1 idi! "el#ti-e humidity
Cuestion# iven the ambient temperature is 1@
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pen!il to the right to read the dew point. This is '@
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for developing an understanding of it,s usage.
The basi! information used to !onstru!t the !hart is the water vapor saturation data
(Tsat 8g) whi!h is obtained from steam tables over the range from Tsat J @.@%
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humidit as a parameter to produ!e the various relative humidit !urves (blue
lines) as follows#
where 8 is the standard atmospheri! pressure %@%.&0' Nk8aO.
The saturation !urve (%@@3 relative humidit) also known as the dew point !urve
is drawn as a red line. Poti!e that on the saturation !urve the wet and dr bulb
temperatures have the same values.
The maFor simplifing assumption in the !onstru!tion of the !hart is that the
enthalp of the mi"ture is assumed to be !onstant throughout the adiabati!
saturation pro!ess. This implies that the evaporating li;uid added does not
signifi!antl affe!t the enthalp of the air4vapor mi"ture leading to the !onstant
slope wet bulb temperature enthalp (red) lines defined b#
Pote that on the L J @ a"is (dr air) h J T N
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where the gas !onstant * air J @.021 NkBkg.9O
It is normal pra!ti!e to separate out the overlapping enthalp wet bulb
temperature lines allowing them to be separatel evaluated. Thus we introdu!e an
obli;ue enthalp a"is and enthalp (bla!k) lines as follows#
The four e;uations highlighted above were programmed in MT?+ and used to
plot the simplified ps!hrometri! !harts shown above.
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Sol-ed %"oblem 5 ssume that the outside air temperature is &0
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Sol-ed %"oblem& Qutside air at &'oneR. Using the 8s!hrometri! =hart neatl plot the re;uired air !onditioning
pro!ess and estimate (a) the amount of moisture removed N%%.'g4H0@kg4dr4air O
(b) the heat removed N(%)4(0) ;!ool J G2kBkg4dr4air O and (!) the amount of heat
added N(0)4(&) ;heat J %@kBkg4dr4air O.
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Sol-ed %"oblem Hot dr air at G@
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This tpe of !ooler is e"tremel popular in hot dr !limates and is popularl
known as a S$#mp 'oole". n interesting appli!ation of using a swamp !ooler to
!ool drinking water in e"tremel hot environments is des!ribed in the posting of
*i!h Qppel in the t :ar blog of the Pew York Times# 6D"i7i! "om Soc7s6.
http://www.consumerenergycenter.org/home/heating_cooling/evaporative.htmlhttp://atwar.blogs.nytimes.com/2009/08/28/drinking-from-socks/http://www.consumerenergycenter.org/home/heating_cooling/evaporative.htmlhttp://atwar.blogs.nytimes.com/2009/08/28/drinking-from-socks/