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4 HVAC Fundamentals:

Psychrometrics

The term moist air is used to emphasize the importance

of both dry air and water vapor in the practice of

HVAC design. Psychrometrics deals with the thermodynamics

of moist air. Although air is made up of a variety

of components, the properties of moist air can be adequately

addressed by considering only the two primary

components, dry air and water vapor. The amount of

moisture in air is very small, and properties are presented

per unit mass of dry air.

FUNDAMENTALS OF MOIST AIR

An important step in the analysis and design of

HVAC systems is to determine the properties of air in

order to provide indoor air quality (IAQ) that promotes

occupant comfort and health. Analysis must include

consideration of the mixture of dry air and varying levels

of moisture. This section reviews fundamental ideal

gas concepts and introduces moist air terminology,

equations, and tools from the ASHRAE Handbook—

Fundamentals (ASHRAE 2005). This chapter summarizes

the equations used to develop the fundamental

graphical tool for moist air analysis and design, the psychrometric

chart. The use of one or more of three

options is allowed:

1. Analysis and design using the psychrometric chart.

2. Analysis and design using packaged psychrometric

software available from vendors or manufacturers.

3. Analysis and design using the psychrometric

spreadsheet (PsychProcess.xls) on the CD that

accompanies this text. This program is in open code

and can be modified to suit additional applications.

Dry air is primarily nitrogen (~78%), oxygen

(~21%), argon (~1%), carbon dioxide (300–400 ppm), 1

and traces of other gases. It has a molecular weight

1. The concentration of carbon dioxide (CO 2 ) in parts per million

(ppm) in outdoor air is important since it has been

widely used in combination with indoor CO 2 concentration

as an indicator of adequate ventilation air.

(MW) of 28.96 lb/lb⋅mole, and the gas constant for air

(R a ) can be determined from the universal gas constant

(R).

R 1545 ( ft ⋅ lb

R a ---------

f ⁄ lb mole ⋅ °R)

= = --------------------------------------------------------------

MW 28.96 ( lb m ⁄ lb mole )

= 53.34 ft ⋅ lbf ⁄ lb m ⋅ °R

(4.1)

The density (ρ) of dry air or its inverse specific volume

(υ = 1/ρ) can be calculated from ideal gas relationships.

At the specified standard conditions of 60°F

(520°R) and sea level atmospheric pressure

(p = 14.696 psia), the specific volume of dry air (υ a ) is

1 R

υ a -- a T 53.34 ( ft ⋅ lbf ⁄ lb

---------

m ⋅ °R) × 520°F

= = = ------------------------------------------------------------------------------

ρ p

14.696 ( lb f ⁄ in. 2 ) × 144 in.2 -------

ft 2

=

13.1 ft 3 ⁄ lb m

(4.2)

The specific volume can be corrected by inserting

an atmospheric pressure corrected for altitude (Z, in feet

above sea level) into Equation 4.2 (ASHRAE 2005).

p (psia) = 14.696 (1 – 6.8753 × 10 –6 Z) 5.2559 (4.3)

It is convenient to express the amount of moisture

in air in terms of the humidity ratio (W), which is the

mass of water vapor (M w ) per mass of dry air (M a ). Current

practice in the US is to use the units of pound mass

of water (lb w ) to pound mass of air (lb a ). Some documents

continue the use of grains per pound mass of air,

where 7000 grains = 1.0 pound mass.

W

M w lb

------- w

lb

------- w

= ≡ ≡ 7000 ( grains ⁄ lb

M a lb w ) × -------

a

lb a

(4.4)

The amount of water vapor required to saturate air

increases with temperature. A widely used term is relative

humidity (RH), which is the mole fraction (or percent)

of water vapor (x w ) present in the air relative to the

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