Trane Air Conditioner trg trc001 en User Manual

Air Conditioning  
Clinic  
Psychrometry  
One of the Fundamental Series  
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The Trane Company • Worldwide Applied Systems Group  
3600 Pammel Creek Road • La Crosse, WI 54601-7599  
An American-Standard Company  
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The Trane Company • Worldwide Applied Systems Group  
3600 Pammel Creek Road • La Crosse, WI 54601-7599  
An American-Standard Company  
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PERMIT NO. 11  
POSTAGE WILL BE PAID BY ADDRESSEE  
THE TRANE COMPANY  
Attn: Applications Engineering  
3600 Pammel Creek Road  
La Crosse WI 54601-9985  
NO POSTAGE  
NECESSARY  
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IN THE  
UNITED STATES  
BUSINESS REPLY MAIL  
LA CROSSE, WI  
FIRST-CLASS MAIL  
PERMIT NO. 11  
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Attn: Applications Engineering  
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Preface  
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Figure 1  
The Trane Company believes that it is incumbent on manufacturers to serve the  
industry by regularly disseminating information gathered through laboratory  
research, testing programs, and field experience.  
The Trane Air Conditioning Clinic series is one means of knowledge sharing. It  
is intended to acquaint a nontechnical audience with various fundamental  
aspects of heating, ventilating, and air conditioning.  
We’ve taken special care to make the clinic as uncommercial and  
straightforward as possible. Illustrations of Trane products only appear in cases  
where they help convey the message contained in the accompanying text.  
This particular clinic introduces the concept of psychrometry, the science  
concerned with the physical laws that govern air – water mixtures.  
© 1999 American Standard Inc. All rights reserved  
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Contents  
period one  
The Psychrometric Chart ................................... 1  
Properties of Air .........................................................2  
Constructing a Simple Psychrometric Chart ..............8  
Effect of Sensible Heat and Moisture Changes .......15  
period two  
Air Mixtures ......................................................... 18  
period three Sensible Heat Ratio ........................................... 22  
period four Air Quantity .......................................................... 30  
period five  
period six  
Tons of Refrigeration ........................................ 37  
Psychrometric Analyses ................................... 42  
period seven Review ................................................................... 52  
Quiz ......................................................................... 57  
Answers ................................................................ 59  
Glossary ................................................................ 64  
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iv  
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period one  
The Psychrometric Chart  
notes  
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Figure 2  
Psychrometry is the science dealing with the physical laws of air – water  
mixtures.  
When designing an air conditioning system, the temperature and moisture  
content of the air to be conditioned, and the same properties of the air needed  
to produce the desired air conditioning effect, must be known. Once these  
properties are known, the air conditioning task can be determined. This analysis  
can be performed using the psychrometric chart. The psychrometric chart  
graphically displays several physical properties of air over a broad range of  
conditions. Knowing the relationship of these air properties aids the task of air  
conditioning system design and analysis.  
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period one  
The Psychrometric Chart  
notes  
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Figure 3  
Properties of Air  
At first glance, the psychrometric chart appears to be an imposing network of  
lines. When properly used, however, it provides valuable information about the  
properties of air. During this session, the psychrometric chart and its use in  
solving many air conditioning problems will be explained.  
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Figure 4  
The psychrometric chart contains five physical properties to describe the  
characteristics of air:  
Dry-bulb temperature  
Wet-bulb temperature  
Dew-point temperature  
Relative humidity  
Humidity ratio  
2
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period one  
The Psychrometric Chart  
notes  
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Figure 5  
Dry-bulb temperatures are read from an ordinary thermometer that has a dry  
bulb.  
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Figure 6  
Wet-bulb temperatures are read from a thermometer whose bulb is covered  
by a wet wick. The difference between the wet-bulb temperature and the dry-  
bulb temperature is caused by the cooling effect produced by the evaporation  
of moisture from the wick. This evaporation effect reduces the temperature of  
the bulb and, therefore, the thermometer reading.  
Consequently, the difference between dry-bulb and wet-bulb temperature  
readings is a measure of the dryness of air. The drier the air, the greater the  
difference between the dry-bulb and wet-bulb readings.  
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period one  
The Psychrometric Chart  
notes  
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Figure 7  
The third property, dew-point temperature, is the temperature at which  
moisture leaves the air and condenses on objects, just as dew forms on grass  
and plant leaves.  
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Figure 8  
When the dry-bulb, wet-bulb, and dew-point temperatures are the same, the air  
is saturated. It can hold no more moisture. When air is at a saturated  
condition, moisture entering the air displaces moisture within the air. The  
displaced moisture leaves the air in the form of fine droplets. When this  
condition occurs in nature, it is called fog.  
4
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period one  
The Psychrometric Chart  
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Figure 9  
The fourth property, relative humidity, is a comparison of the amount of  
moisture that a given amount of air is holding, to the amount of moisture that  
the same amount of air can hold, at the same dry-bulb temperature.  
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Figure 10  
Relative humidity is expressed as a percentage. For example, if the relative  
humidity of the air is 50%, it contains one-half the amount of moisture possible  
at the existing dry-bulb temperature.  
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period one  
The Psychrometric Chart  
notes  
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Figure 11  
Finally, humidity ratio describes the actual weight of water in an air – water  
vapor mixture. In other words, if one pound of air were wrung completely dry,  
comparing the weight of the water to the weight of the dry air would yield its  
humidity ratio.  
Humidity ratio can be expressed as pounds of moisture per pound of dry air, or  
as grains of moisture per pound of dry air. There are 7000 grains of water in a  
pound. To appreciate the magnitude of these units of measurement, at sea level  
one pound of 70°F air occupies approximately 13.5 cubic feet, and one grain of  
water in that air weighs about two-thousandths (0.002) of an ounce.  
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Figure 12  
When any two of these five properties of air are known, the other three can be  
quickly determined from the psychrometric chart.  
6
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period one  
The Psychrometric Chart  
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Figure 13  
For example, let's assume that the summer design conditions are 95°F dry bulb  
and 78°F wet bulb.  
What is the relative humidity, humidity ratio, and dew point?  
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Only one point on the psychrometric chart represents air with both of these  
conditions. This point is located where the vertical 95°F dry-bulb (DB) and  
diagonal 78°F wet-bulb (WB) temperature lines intersect.  
From this intersection, the remaining three air properties can be read from the  
chart. Both the dew-point and humidity-ratio lines are horizontal and the values  
are shown on the right side of the chart. In this example, the humidity ratio is  
about 118 grains of moisture per pound of dry air and the dew-point  
temperature is approximately 72°F.  
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period one  
The Psychrometric Chart  
Notice that the point of intersection falls between two relative humidity curves:  
40% and 50%. By interpolation, the relative humidity at this condition is  
approximately 47%.  
notes  
Constructing a Simple Psychrometric Chart  
To better understand the psychrometric chart and show why the lines intersect  
as they do, we will construct a simple chart.  
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Figure 15  
The amount of moisture contained in saturated air depends on dry-bulb  
temperature. This table shows the maximum amount of water vapor that one  
pound of dry air can hold at various dry-bulb temperatures. For example, at  
25°F, one pound of dry air can absorb and hold 19.14 grains of water; at 30°F it  
can absorb 24.19 grains; at 35°F it can absorb 29.94 grains; and so on. Each of  
these conditions is a saturation point.  
8
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period one  
The Psychrometric Chart  
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These saturation points can be plotted on a chart with dry-bulb temperature  
along the horizontal axis and humidity ratio along the vertical axis.  
When several saturation points are plotted, the curve created resembles the  
relative humidity curves of the psychrometric chart.  
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In fact, this curve forms the 100% relative-humidity curve or saturation curve.  
All points on this curve represent the moisture content that constitutes  
complete saturation of air at the various dry-bulb temperatures.  
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period one  
The Psychrometric Chart  
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Another fact about saturated air should be discussed before we proceed.  
Assume a volume of moist air has the initial conditions indicated in column D  
of the table. The air has a 90°F dry-bulb temperature and a 60°F dew point. A  
wet-bulb thermometer shows the wet-bulb temperature to be 70°F. From a  
moisture-content table, the relative humidity of the air is approximately 37%.  
With no change in the moisture content of this volume of air, the table shows  
the progressive change that occurs as the air cools.  
Point C: As the dry-bulb temperature drops from 90°F to 75°F, the wet-bulb  
temperature drops from 70°F to 65.2°F, yet the dew point remains the same at  
60°F. The relative humidity rises from 37% to 60%.  
Point B: When the dry-bulb temperature reaches 62°F, the wet-bulb  
temperature is about 60.8°F, the dew point remains constant at 60°F, and the  
relative humidity is 92%.  
Point A: Finally, when the dry-bulb temperature reaches the 60°F dew-point  
temperature, the wet bulb cannot be reduced any lower because evaporation  
can no longer occur: the air is saturated and contains all the moisture it can  
hold. The relative humidity is now 100%.  
At any point on a 100% relative-humidity curve, the three air  
temperatures—dry bulb, wet bulb and dew point—are equal.  
10  
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period one  
The Psychrometric Chart  
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Figure 19  
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Additionally, the dew-point temperature does not change as the dry-bulb  
temperature changes, provided that the moisture content of the air remains the  
same. Merely heating the air does not change its moisture content. Therefore,  
as the air is heated, its condition will move horizontally along a constant  
humidity-ratio line.  
In this example, heating 60°F saturated air moves the air condition along a  
horizontal humidity-ratio line that corresponds to a constant 77.56 grains of  
moisture per pound of dry air.  
Horizontal lines can be drawn from each saturation point across to the right  
side of the chart. A horizontal line can be provided for each humidity-ratio  
value.  
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period one  
The Psychrometric Chart  
notes  
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Additional curves can be added to the chart to represent relative humidity  
conditions that are less than 100%. The curves shown are at 10% intervals and  
represent humidity conditions ranging from completely saturated air to  
completely dry air. When air is completely dry, its relative humidity cannot  
change with temperature. The 0% condition is therefore represented by the  
horizontal axis of the chart.  
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Figure 21  
'U\ꢀ%XOEꢂ7HPSHUDWXUHꢂꢅƒ)ꢆ  
This basic chart now shows three air conditions: dry-bulb temperature (vertical  
lines), humidity ratio (horizontal lines) and relative humidity (diagonally curved  
lines).  
12  
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period one  
The Psychrometric Chart  
notes  
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Figure 22  
'U\ꢀ%XOEꢂ7HPSHUDWXUHꢂꢅƒ)ꢆ  
To complete this basic chart, the wet-bulb temperature lines must be added.  
Once again, at a saturated condition the wet-bulb, dry-bulb and dew-point  
temperatures are equal. Therefore, the wet-bulb temperature lines start at the  
saturation curve.  
To observe what happens to wet-bulb temperatures when air is heated, start  
with saturated air at 50°F dry bulb. At this condition, the air has a moisture  
content of approximately 54 grains per pound as shown by A. If the  
temperature of this air is increased to 75°F dry bulb without changing its  
moisture content, the air condition will move along the constant humidity ratio  
line (54 grains/lb) to B. The wet-bulb temperature of this warmed air is  
approximately 60.1°F.  
A line drawn from B to a point on the saturation curve that represents 60.1°F  
saturation temperature (B’) gives an indication of the direction the wet-bulb  
temperature lines will run. By taking numerous wet-bulb readings under  
different conditions, the wet-bulb temperature lines can be added to the chart.  
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period one  
The Psychrometric Chart  
notes  
3URSHUWLHVꢀRIꢀ$LU  
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GU\ꢂEXOE  
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Figure 23  
'U\ꢀ%XOEꢂ7HPSHUDWXUHꢂꢅƒ)ꢆ  
The psychrometric chart now defines these five properties of air: dry-bulb  
temperature (vertical lines), humidity ratio and dew-point temperature  
(horizontal lines), relative humidity (curved lines) and wet-bulb temperature  
(diagonal lines).  
Remember: if any two of these five air conditions are known, the other three  
can be found on the psychrometric chart by locating the point of intersection of  
the two known conditions.  
6SHFLILFꢀ9ROXPH  
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ꢂꢂꢅFXELFꢂIHHWꢂꢇꢂSRXQGꢂRIꢂGU\ꢂDLUꢆ  
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Figure 24  
'U\ꢀ%XOEꢂ7HPSHUDWXUHꢂꢅƒ)ꢆ  
There is one more property of air that is displayed on the psychrometric chart—  
specific volume. Specific volume is defined as the volume of one pound of  
dry air at a specific temperature and pressure. As one pound of air is heated it  
occupies more space—the specific volume increases.  
14  
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period one  
The Psychrometric Chart  
notes  
(IIHFWꢀRIꢀ$GGLQJꢀ6HQVLEOHꢀ+HDW  
Figure 25  
Effect of Sensible Heat and Moisture Changes  
When either the sensible heat content or the moisture content of air changes,  
the point on the psychrometric chart that represents the original air condition  
moves to a position that represents the new condition of temperature and/or  
humidity.  
For example, if sensible heat is added to air, the air condition moves  
horizontally to the right.  
(IIHFWꢀRIꢀ5HPRYLQJꢀ6HQVLEOHꢀ+HDW  
Figure 26  
Conversely, if sensible heat is removed from air, the air condition moves  
horizontally to the left. As long as the moisture content of the air remains  
unchanged, the humidity ratio remains the same. Therefore, this movement  
follows the horizontal humidity-ratio lines.  
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period one  
The Psychrometric Chart  
notes  
(IIHFWꢀRIꢀ$GGLQJꢀ0RLVWXUH  
Figure 27  
On the other hand, if moisture is added to air without changing the dry-bulb  
temperature, the air condition moves upward along a dry-bulb temperature  
line.  
(IIHFWꢀRIꢀ5HPRYLQJꢀ0RLVWXUH  
Figure 28  
Finally, if moisture is removed from the air without changing its dry-bulb  
temperature, the air condition moves downward along a dry-bulb temperature  
line.  
16  
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period one  
The Psychrometric Chart  
notes  
5HPRYLQJꢀ6HQVLEOHꢀ+HDWꢀDQGꢀ0RLVWXUH  
Figure 29  
Put all of these changes together on one chart and they show the direction the  
air condition will move when the dry-bulb temperature or moisture content is  
altered.  
5HPRYLQJꢀ6HQVLEOHꢀ+HDWꢀDQGꢀ0RLVWXUH  
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Figure 30  
In actual practice, however, both the dry-bulb temperature and moisture  
content of the air generally change simultaneously. When this happens, the  
resulting air conditions move from A at some angle. The exact angle and  
direction depend upon the proportions of sensible and latent heat added or  
removed. Sensible heat causes a change in the air’s dry-bulb temperature  
with no change in moisture content. Latent heat causes a change in the air’s  
moisture content with no change in dry-bulb temperature.  
To provide summer comfort, air is cooled and dehumidified, moving the air  
condition downward and to the left, resulting in a lower dry-bulb temperature  
and a lower moisture content.  
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period two  
Air Mixtures  
notes  
3V\FKURPHWU\  
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Figure 31  
Before an air conditioning problem can be analyzed on the psychrometric chart,  
the conditions of the air to be cooled or heated must be known.  
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Figure 32  
The air entering the cooling coil may be 100% recirculated (A), 100% outdoor  
(B), or a mixture of the two (C).  
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period two  
Air Mixtures  
notes  
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Figure 33  
If outdoor air B is mixed with recirculated air A, the conditions of the resulting  
mixture are found somewhere on a straight line connecting the two points.  
If the mixture is half and half, this condition falls on the midpoint of the line  
between A and B. If more than half of the mixture is recirculated air A, the  
condition of the mixture will fall closer to A than to B.  
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Figure 34  
In this example, 1,000 cfm of outdoor air (OA) is mixed with 3,000 cfm of  
recirculated air (RA) for a total supply airflow of 4,000 cfm.  
First, the percentage of outdoor air within the mixture is determined. This is  
done by dividing the outdoor air quantity by the total air quantity.  
1,000 cfm  
4,000 cfm  
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= 0.25  
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period two  
Air Mixtures  
The outdoor air quantity in this example constitutes 25% of the mixture, while  
the recirculated air makes up the remaining 75%.  
notes  
The next step is to determine the dry-bulb temperature of the air mixture.  
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Figure 35  
This is done by multiplying the dry-bulb temperature of each air condition by its  
percentage and summing the results.  
For example, if the outdoor dry-bulb temperature is 95°F and it represents 25%  
of the air mixture, it contributes 23.75°F (or 0.25 × 95) to the dry-bulb  
temperature of the air mixture.  
Similarly, if the dry-bulb temperature of the recirculated air is 80°F, it  
contributes 60°F (or 0.75 × 80) to the dry-bulb temperature of the air mixture.  
The sum of 23.75°F and 60°F equals 83.75°F, the resulting dry-bulb temperature  
of this air mixture.  
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period two  
Air Mixtures  
notes  
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Figure 36  
Returning to the psychrometric chart, point C, at which the 83.75°F dry-bulb  
temperature falls on the line from A to B, represents the conditions of the air  
mixture: 83.75°F DB and approximately 70°F WB.  
Because the recirculated air quantity constitutes a larger percentage (75%) of  
the mixture, the mixed-air condition (C) is much nearer to the indoor design  
condition (A) than to the outdoor design condition (B).  
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period three  
Sensible Heat Ratio  
notes  
3V\FKURPHWU\  
SHULRGꢀWKUHH  
6HQVLEOHꢀ+HDWꢀ5DWLR  
Figure 37  
This period is devoted to understanding the term sensible heat ratio and how  
it is represented on the psychrometric chart. The ratio of sensible heat gain to  
total heat gain is one of the most important factors affecting air conditioning  
system requirements.  
(IIHFWꢀRIꢀ5HPRYLQJꢀ6HQVLEOHꢀ+HDW  
Figure 38  
If only sensible heat is removed from the air, the line representing this change  
moves from the original condition horizontally to the left. This results in a lower  
dry-bulb temperature, while the moisture content (the humidity ratio) remains  
constant.  
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period three  
Sensible Heat Ratio  
notes  
(IIHFWꢀRIꢀ5HPRYLQJꢀ/DWHQWꢀ+HDW  
Figure 39  
Conversely, if only latent heat is removed, the line moves vertically downward  
along a constant dry-bulb temperature line. This results in a lower moisture  
content or humidity ratio.  
5HPRYLQJꢀ6HQVLEOHꢀDQGꢀ/DWHQWꢀ+HDW  
Figure 40  
If both sensible and latent heat are removed from the air, the resulting air  
condition will be to the left and below the initial condition. The proportions of  
sensible and latent heat removed will determine the exact direction the  
resulting air condition follows.  
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period three  
Sensible Heat Ratio  
notes  
+HDWꢀDQGꢀ0RLVWXUHꢀ7UDQVIHU  
VXSSO\ꢂDLU  
UHWXUQꢂDLU  
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Figure 41  
Imagine conditioned supply air as a sponge. As it enters a room, it absorbs heat  
and moisture. The amount of heat and moisture absorbed depends on the  
temperature and humidity of the supply air. This “sponge,” the supply air, must  
be cool enough to pick up the room's excess sensible heat gain and dry enough  
to pick up the room's excess latent heat (i.e., moisture.)  
Therefore, the excess sensible and latent heat in the room determine the  
required dry-bulb and wet-bulb temperatures of that supply air.  
24  
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period three  
Sensible Heat Ratio  
notes  
5HPRYLQJꢀ6HQVLEOHꢀDQGꢀ/DWHQWꢀ+HDW  
FRROHUꢂ ꢂGDPSHU  
FRROHUꢂ ꢂGDPSHU  
ZDUPHUꢂ ꢂGULHU  
ZDUPHUꢂ ꢂGULHU  
Figure 42  
When the required amount of sensible and latent heat are not properly  
removed from the room, the desired room conditions cannot be maintained.  
For example, if too much sensible heat and not enough latent heat are  
removed, the room feels cold and damp. On the psychrometric chart, room  
conditions move up and to the left.  
On the other hand, if too much latent heat but not enough sensible heat is  
removed, the room feels warm and dry. On the psychrometric chart, room  
conditions move down and to the right.  
Therefore, the conditions of the supply air must be controlled accurately to  
ensure that both sensible and latent heat are removed in the proper  
proportions. There are several combinations of dry-bulb and wet-bulb  
temperatures that will produce the desired room conditions. Each of these  
combinations requires a different quantity of air.  
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period three  
Sensible Heat Ratio  
notes  
+HDWꢀ*DLQ  
Figure 43  
This relationship between the conditions and quantity of the supply air can be  
described using the analogy of maintaining a constant temperature within a  
container of water.  
In this illustration, the container of water is capable of absorbing heat. The  
amount of heat it absorbs is called heat gain. To maintain the water  
temperature at a constant 75°F, any heat gain must be offset by mixing cool  
water with the water already in the container.  
The rate at which this cool water is added to the container is determined by its  
temperature. For a given water temperature there is a certain flow rate—  
measured in gallons per minute (gpm)—that will offset the heat gain and  
maintain the desired temperature in the container. If the water is warm, a higher  
flow rate is required than if the water is very cold.  
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period three  
Sensible Heat Ratio  
notes  
6HQVLEOHꢀ+HDWꢀ5DWLRꢀꢆ6+5ꢇ  
6HQVLEOHꢀ+HDWꢀ*DLQ  
6+5   
6HQVLEOHꢀ+HDWꢀ*DLQꢀꢑꢀ/DWHQWꢀ+HDWꢀ*DLQ  
Figure 44  
The sensible heat ratio, abbreviated as SHR, refers to the comparison of  
sensible heat gain to total heat gain (sensible heat plus latent heat). Once this  
ratio is known, an SHR line can be drawn on the psychrometric chart.  
Sensible Heat Gain  
Sensible Heat Gain + Latent Heat Gain  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
Sensible Heat Ratio (SHR) =  
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LQGH[ꢂSRLQW  
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L
Figure 45  
A scale around the right and top edges of the chart gives the SHR values. Also,  
there is an index point in the middle of the chart at the 78°F DB and 65°F WB  
condition.  
Using a straight edge, a sensible heat ratio line can be drawn by aligning the  
appropriate SHR value on the scale with the index point.  
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period three  
Sensible Heat Ratio  
notes  
'UDZLQJꢀDQꢀ6+5ꢀ/LQH  
$
$
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L
L
Figure 46  
Assume that room design conditions (A) are 78°F DB and 65°F WB, and that the  
sensible heat ratio is calculated as 0.80. That is, sensible heat gain represents  
80% of the total (sensible plus latent) heat gain.  
The SHR line is found by aligning the index point with the 0.80 marking on the  
sensible-heat-ratio scale and drawing a line from the index point to the  
saturation curve.  
6+5ꢀ'LFWDWHVꢀ6XSSO\ꢀ$LUꢀ&RQGLWLRQ  
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Figure 47  
Supply air with any combination of dry-bulb and wet-bulb temperatures that  
falls on this line will be able to absorb the room's sensible and latent heat in the  
correct proportions needed to maintain the desired room conditions  
(A = 78°F DB, 65°F WB).  
Each of these combinations, however, requires a different quantity of air to do  
the task. Recall the analogy with the container of water. If the supply air is  
warm, a higher quantity of air is required than if the supply air is cold.  
28  
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period three  
Sensible Heat Ratio  
notes  
'UDZLQJꢀDQꢀ6+5ꢀ/LQH  
%
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Figure 48  
Sensible-heat-ratio lines for other conditions are drawn in the following  
manner. Assume that room design conditions are 80°F DB and 60% RH, and  
that the SHR is calculated as 0.60.  
First, line up the index point with the 0.60 marking on the sensible-heat-ratio  
scale and draw a line. Next, draw a second line, parallel to the first, through the  
point (B) that represents the design room conditions. This is the 0.60 SHR line  
for a room at 80°F DB and 60% RH.  
Supply air at C (60°F DB and 58°F WB) will maintain the desired room  
conditions, as will supply air at D (70°F DB and 64°F WB). To do so, each of  
these combinations will require a different quantity of air.  
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period four  
Air Quantity  
notes  
3V\FKURPHWU\  
SHULRGꢀIRXU  
$LUꢀ4XDQWLW\  
Figure 49  
Next, we will determine the flow rate of supply air necessary to maintain a  
given set of design room conditions.  
&RLOꢀ&XUYHV  
FRLOꢂFXUYHV  
FRLOꢂFXUYHV  
Figure 50  
Before proceeding, one more set of curves on the psychrometric chart must be  
identified. These curved lines represent the changes in dry-bulb and wet-bulb  
temperatures as air passes through a “typical” cooling coil. These are  
commonly referred to as coil curves; they depict approximate coil  
performance. Exact coil performance depends on the actual coil geometry and  
can be precisely determined by coil selection software.  
These curves were established from hundreds of laboratory tests of various coil  
geometries at different air and coolant temperatures. They let you determine  
leaving-coil conditions and postpone coil selection until the final design. The  
use of these coil curves will be discussed later.  
30  
TRG-TRC001-EN  
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period four  
Air Quantity  
notes  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
67(3ꢀꢅꢓꢀꢀ&DOFXODWHꢀWKHꢀVHQVLEOHꢀKHDWꢀUDWLRꢀꢆ6+5ꢇ  
ꢊꢃꢐꢃꢃꢃꢀ%WXꢒKUꢀVHQVLEOHꢀKHDWꢀJDLQ  
ꢌꢃꢐꢃꢃꢃꢀ%WXꢒKUꢀODWHQWꢀKHDWꢀJDLQ  
ꢊꢃꢐꢃꢃꢃꢀ%WXꢒKU  
6+5  
 
 
ꢃꢎꢊꢃ  
ꢅꢃꢃꢐꢃꢃꢃꢀ%WXꢒKU  
Figure 51  
To demonstrate how the required supply airflow is determined, assume that a  
room’s sensible heat gain is 80,000 Btu/hr and its latent heat gain is 20,000 Btu/  
hr. First, divide the sensible heat gain by the total heat gain. The resulting  
sensible heat ratio (SHR) is 0.80.  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
URRPꢀ¥ꢀꢉꢊƒ)ꢀ'%ꢐꢀꢂꢃꢄꢀ5+  
RXWGRRUꢀDLUꢀꢆ2$ꢇꢀ¥ꢀꢈꢂƒ)ꢀ'%ꢐꢀꢉꢊƒ)ꢀ:%  
YHQWLODWLRQꢀ¥ꢀꢌꢂꢄꢀ2$  
Figure 52  
The second step is to determine the entering air conditions. Design room air is  
78°F DB, 50% RH; design outdoor air is 95°F DB, 78°F WB  
Twenty-five percent (25%) outdoor air is required for ventilation purposes.  
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31  
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period four  
Air Quantity  
notes  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
67(3ꢀꢌꢓꢀꢀ3ORWꢀURRPꢐꢀRXWGRRUꢐꢀDQGꢀHQWHULQJꢀFRQGLWLRQV  
ꢈꢂƒ)ꢀÕꢀꢃꢎꢌꢂꢀ ꢀꢌꢍꢎꢉꢂƒ)  
ꢉꢊƒ)ꢀÕꢀꢃꢎꢉꢂꢀ ꢀꢂꢊꢎꢂꢃƒ)  
PL[WXUHꢀ ꢀꢊꢌꢎꢌꢂƒ)  
%
&
$
Figure 53  
Plot the outdoor air B (95°F DB, 78°F WB) and indoor air A (78°F DB, 65°F WB)  
conditions on the psychrometric chart. Then calculate the mixed-air conditions  
using the method learned in Period 2.  
95°F × 0.25 = 23.75°F  
78°F × 0.75 = 58.50°F  
Mixed-Air Temperature = 23.75°F + 58.50°F = 82.25°F  
Locate the mixed air conditions C on the psychrometric chart (82.25°F DB,  
68.6°F WB).  
Next, establish the SHR line by aligning the 0.80 mark on the scale with the  
index point and drawing a line through both points to the saturation curve. In  
this case, the room design conditions and the index point are the same  
(A = 78°F DB, 65°F WB).  
32  
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period four  
Air Quantity  
notes  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
67(3ꢀꢍꢓꢀꢀ,GHQWLI\ꢀVXSSO\ꢀDLUꢀFRQGLWLRQV  
%
&
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ꢂꢏꢎꢂƒ)  
ꢉꢊƒ)  
Figure 54  
The third step is to determine the required supply air conditions. This is where  
the coil curves are used. Using the curvature of the nearest coil line as a guide,  
draw a curve from the mixed-air condition C until it intersects the SHR line.  
Point D, at which this curve crosses the SHR line, represents the supply air  
condition that will absorb the room’s sensible and latent heat in the correct  
proportions needed to maintain the desired room conditions. Here, this supply  
air condition is found to be 56.5°F DB and 55.2°F WB.  
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period four  
Air Quantity  
notes  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
67(3ꢀꢋꢓꢀꢀ6ROYHꢀWKHꢀVXSSO\ꢀDLUIORZꢀHTXDWLRQ  
6HQVLEOHꢀ+HDWꢀ*DLQ  
6XSSO\  
 
$LUIORZ  
ꢅꢎꢃꢊꢂꢀÕꢀꢆ5RRPꢀ'%ꢀ¤ꢀ6XSSO\ꢀ'%ꢇ  
Figure 55  
With the supply air conditions known, the next step is to calculate the specific  
quantity of air (cfm or cubic feet per minute) needed to satisfy the room heat  
gains. The required supply airflow is determined using the following formula,  
where the sensible heat gain is expressed in Btu/hr and the two temperatures  
are in °F.  
Sensible Heat Gain  
1.085 × (Room DB Supply DB)  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
Supply Airflow (cfm) =  
Realize that 1.085 is not a constant! It is the product of density, the specific heat  
of air and the conversion factor of 60 minutes per hour. These properties of air  
at “standard” conditions (69.5°F DB dry air at sea level) result in the value  
1.085. Air at other conditions and elevations will cause this factor to change.  
Density = 0.075 lb/ft3  
Specific Heat = 0.24 Btu/lb°F  
0.075 × 0.24 × 60 min/hr = 1.085  
34  
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period four  
Air Quantity  
notes  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
67(3ꢀꢋꢓꢀꢀ6ROYHꢀWKHꢀVXSSO\ꢀDLUIORZꢀHTXDWLRQ  
ꢊꢃꢐꢃꢃꢃꢀ%WXꢒKU  
  ꢍꢐꢋꢍꢃꢀFIP  
ꢅꢎꢃꢊꢂꢀÕꢀꢆꢉꢊƒ)ꢀ¤ꢀꢂꢏꢎꢂƒ)  
Figure 56  
For this example, the supply airflow is calculated as follows:  
80,000 Btu/hr  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
Supply Airflow (cfm) =  
= 3,430 cfm  
1.085 × (75°F 56.5°F)  
'HWHUPLQLQJꢀ6XSSO\ꢀ$LUIORZ  
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2$  
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5$  
Figure 57  
The cooling coil must cool and dehumidify 3,430 cfm of air from the entering  
condition C to the supply air condition D to maintain the desired room  
conditions.  
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35  
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period four  
Air Quantity  
notes  
$UELWUDULO\ꢀ8VLQJꢀꢂꢂƒ)ꢀ6XSSO\ꢀ$LU  
ꢋꢉꢐꢃꢃꢃꢀ%WXꢒKUꢀVHQVLEOHꢀKHDWꢀJDLQ  
ꢌꢃꢐꢃꢃꢃꢀ%WXꢒKUꢀODWHQWꢀKHDWꢀJDLQ  
ꢋꢉꢐꢃꢃꢃꢀ%WXꢒKU  
6+5  
 
 
ꢃꢎꢉꢃ  
ꢏꢉꢐꢃꢃꢃꢀ%WXꢒKU  
Figure 58  
Some designers prefer to set the supply air temperature at 55°F or use a 20°F  
temperature differential (Room DB – Supply DB) without regard for the actual  
sensible heat ratio of the room.  
Using our same example, let’s examine how this has the potential for creating a  
problem. Assume that the building design changes to use a much-higher-  
quality glass that will reduce the sensible portion of the design load from  
80,000 Btu/hr to 47,000 Btu/hr. This reduces the SHR to 0.70.  
$UELWUDULO\ꢀ8VLQJꢀꢂꢂƒ)ꢀ6XSSO\ꢀ$LU  
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Figure 59  
Plotting this new SHR line on the psychrometric chart, we find that the SHR line  
crosses the coil curve at approximately 49°F DB (D).  
If the system is arbitrarily designed with a 55°F supply air temperature D’, the  
resulting room conditions will fall on the 0.70 SHR line drawn through D’. The  
resulting room conditions A’ will be 78°F DB, 57% RH. This arbitrary design  
practice results in a higher room relative humidity than desired.  
36  
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period five  
Tons of Refrigeration  
notes  
3V\FKURPHWU\  
SHULRGꢀILYH  
7RQVꢀRIꢀ5HIULJHUDWLRQ  
Figure 60  
The psychrometric chart can also be used to determine the total load on the  
refrigeration equipment, expressed in Btu per hour or tons of refrigeration.  
One ton equals 12,000 Btu/hr.  
:KDWꢀLVꢀ(QWKDOS\"  
7KHꢀWRWDOꢀKHDWꢀHQHUJ\ꢀLQꢀRQHꢀSRXQGꢀRIꢀDLU  
ꢁ%WXꢂOEꢃꢀDWꢀLWVꢀSUHVHQWꢀFRQGLWLRQꢄ  
(QWKDOS\ꢀꢆKꢇꢀ ꢀ6HQVLEOHꢀ+HDWꢀꢑꢀ/DWHQWꢀ+HDW  
Figure 61  
Another property of air, enthalpy, must now be defined. Enthalpy describes the  
total amount of heat energy, both sensible and latent, in one pound of air at its  
present condition. It is expressed in Btu per pound of dry air (Btu/lb). When  
displayed in formulas, enthalpy is usually designated as h.  
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period five  
Tons of Refrigeration  
notes  
'HWHUPLQLQJꢀ7RQVꢀRIꢀ5HIULJHUDWLRQ  
67(3ꢀꢅꢓꢀ  
)LQGꢀHQWKDOSLHV  
HQWHULQJꢀDQG  
OHDYLQJꢀFRLO  
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Figure 62  
Using the previous example for calculating supply airflow, the first step is to  
determine the enthalpies of the air entering and leaving the cooling coil. This is  
accomplished by lining up three points on the chart, including the entering-air  
condition and identical points on the two enthalpy scales—one each on the left  
and right edges of the psychrometric chart.  
Using this method, the enthalpy of the mixed air entering the coil C is found to  
be 32.7 Btu/lb. Similarly, the enthalpy of the supply air leaving the coil D is  
found to be 23.5 Btu/lb.  
'HWHUPLQLQJꢀ7RQVꢀRIꢀ5HIULJHUDWLRQ  
67(3ꢀꢌꢓꢀꢀ6ROYHꢀWKHꢀWRWDOꢀUHIULJHUDWLRQꢀORDGꢀHTXDWLRQ  
5HIULJHUDWLRQ  
/RDGꢀꢆ%WXꢒKUꢇ  
ꢋꢎꢂꢀÕꢀ6XSSO\ꢀ$LUIORZꢀÕꢀK ꢀ¤ꢀK  
 
Kꢀꢀ ꢀꢀHQWKDOS\ꢀRIꢀDLUꢀHQWHULQJꢀFRLOꢀꢆ%WXꢒOEꢇ  
Kꢀꢀ ꢀꢀHQWKDOS\ꢀRIꢀDLUꢀOHDYLQJꢀFRLOꢀꢆ%WXꢒOEꢇ  
Figure 63  
The total refrigeration load, in terms of Btu per hour, is then calculated using  
the following formula, where the supply airflow is expressed in cfm, h1 is the  
entering-air enthalpy in Btu/lb, and h2 is the leaving-air enthalpy in Btu/lb.  
Refrigeration Load (Btu/hr) = 4.5 × Supply Airflow × (h1 h2)  
38  
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period five  
Tons of Refrigeration  
Realize that 4.5 is not a constant! It is the product of density of air and the  
conversion factor of 60 minutes per hour. The density of air at “standard”  
conditions (69.5°F DB dry air at sea level) results in the value 4.5. Air at other  
conditions and elevations will cause this factor to change.  
notes  
Density = 0.075 lb/ft3  
0.075 × 60 min/hr = 4.5  
'HWHUPLQLQJꢀ7RQVꢀRIꢀ5HIULJHUDWLRQ  
67(3ꢀꢌꢓꢀꢀ6ROYHꢀWKHꢀWRWDOꢀUHIULJHUDWLRQꢀORDGꢀHTXDWLRQ  
ꢋꢎꢂꢀÕꢀꢍꢐꢋꢍꢃꢀFIPꢀÕꢀꢆꢍꢌꢎꢉꢀ¤ꢀꢌꢍꢎꢂꢇꢀ ꢅꢋꢌꢐꢃꢃꢃꢀ%WXꢒKU  
ꢅꢋꢌꢐꢃꢃꢃꢀ%WXꢒKU  
 ꢀꢅꢅꢎꢊꢀWRQVꢀRIꢀUHIULJHUDWLRQ  
ꢅꢌꢐꢃꢃꢃꢀ%WXꢒKUꢒWRQ  
Figure 64  
Using the supply airflow calculated during Period 4 and the enthalpy values  
read from the psychrometric chart:  
Refrigeration Load (Btu/hr = 4.5 × 3,430 cfm × (32.7 23.5) = 142,000 Btu/hr  
Converting to the more common units of tons:  
142,000 Btu/hr  
12,000 Btu/hr/ton  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
= 11.8 tons of refrigeration  
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period five  
Tons of Refrigeration  
notes  
6HQVLEOHꢀDQGꢀ/DWHQWꢀ&RLOꢀ/RDGV  
ODWHQW  
ꢂORDG  
%
%
VHQVLEOH  
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Figure 65  
The psychrometric chart can also be used to determine the sensible and latent  
components of the coil’s refrigeration load.  
First, draw a right triangle though the coil entering and leaving air conditions.  
The vertical leg represents the amount of moisture removed by the coil, i.e.,  
latent load, and the horizontal leg represents the amount of change in dry-bulb  
temperature through the coil, i.e., sensible load.  
40  
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period five  
Tons of Refrigeration  
notes  
6HQVLEOHꢀDQGꢀ/DWHQWꢀ&RLOꢀ/RDGV  
ꢋꢎꢂꢀÕꢀꢍꢐꢋꢍꢃꢀFIPꢀÕꢀꢆꢌꢈꢎꢏꢀ¤ꢀꢌꢍꢎꢂꢇꢀ ꢀꢈꢋꢐꢅꢂꢃꢀ%WXꢒKU  
ꢉꢎꢊꢀWRQVꢀRIꢀUHIULJHUDWLRQꢀꢆVHQVLEOHꢇ  
ꢋꢎꢂꢀÕꢀꢍꢐꢋꢍꢃꢀFIPꢀÕꢀꢆꢍꢌꢎꢉꢀ¤ꢀꢌꢈꢎꢏꢇꢀ ꢋꢉꢐꢊꢂꢃꢀ%WXꢒKU  
ꢋꢎꢃꢀWRQVꢀRIꢀUHIULJHUDWLRQꢀꢆODWHQWꢇ  
Figure 66  
By determining the enthalpy values for these three points, the same equation  
can be used to calculate both the sensible and the latent portions of the coil’s  
refrigeration load.  
Sensible Refrigeration Load = 4.5 × 3,430 cfm × (29.6 23.5) = 94,150 Btu/hr  
94,150 Btu/hr  
12,000 Btu/hr/ton  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
= 7.8 tons of refrigeration (sensible)  
Latent Refrigeration Load = 4.5 × 3,430 cfm × (32.7 29.6) = 47,850 Btu/hr  
47,850 Btu/hr  
12,000 Btu/hr/ton  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
= 4.0 tons of refrigeration (latent)  
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period six  
Psychrometric Analyses  
notes  
3V\FKURPHWU\  
SHULRGꢀVL[  
3V\FKURPHWULFꢀ$QDO\VHV  
Figure 67  
Now we will look at a few ways that the psychrometric chart can help us  
analyze air conditioning systems. For simplicity, we will limit our examples to  
systems serving a single zone.  
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Figure 68  
In the previous example, the sensible heat ratio was based on full load or  
design load conditions. It must be understood that the sensible portion of  
total heat gain is particularly subject to change throughout the day, causing the  
ratio of sensible to total heat gain to change.  
42  
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period six  
Psychrometric Analyses  
notes  
6+5ꢀ&KDQJHVꢀZLWKꢀ5RRPꢀ/RDG  
)XOOꢁ/RDGꢀ6+5ꢓ  
ꢊꢃꢐꢃꢃꢃꢀ%WXꢒKU  
 ꢀꢀꢃꢎꢊꢃ  
ꢊꢃꢐꢃꢃꢃꢀ%WXꢒKUꢀꢑꢀꢌꢃꢐꢃꢃꢃꢀ%WXꢒKUꢀ  
3DUWꢁ/RDGꢀ6+5ꢓ  
ꢋꢉꢐꢃꢃꢃꢀ%WXꢒKU  
 ꢀꢀꢃꢎꢉꢃ  
ꢋꢉꢐꢃꢃꢃꢀ%WXꢒKUꢀꢑꢀꢌꢃꢐꢃꢃꢃꢀ%WXꢒKUꢀ  
Figure 69  
For example, assume that at full load the room is subject to an 80,000 Btu/hr  
sensible heat gain and a 20,000 Btu/hr latent heat gain. The full-load sensible  
heat ratio is 0.80.  
At other times during the day, clouds block the sun and reduce the solar heat  
gain, and some of the lights are turned off. This reduces the room’s sensible  
heat gain from 80,000 Btu/hr to 47,000 Btu/hr. The room’s latent heat gain  
originates primarily from people. Assuming that the occupancy of the room  
remains constant, the latent heat gain is still 20,000 Btu/hr and the part-load  
sensible heat ratio becomes 0.70.  
6+5ꢀDWꢀ3DUWꢁ/RDGꢀ&RQGLWLRQV  
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Figure 70  
To maintain the design room conditions A for this part-load sensible heat ratio,  
a different supply air condition—one that falls on the 0.70 SHR line—and a  
different airflow are required. But suppose the system in this example was  
designed to deliver a constant quantity of air and vary its supply temperature to  
meet the changing loads.  
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period six  
Psychrometric Analyses  
notes  
6+5ꢀDWꢀ3DUWꢁ/RDGꢀ&RQGLWLRQV  
ꢇꢊꢆꢀꢀꢀꢃ%WXꢋKU  
 ꢃꢅꢆꢇꢅꢀꢃFIP  
ꢌꢁꢀꢂꢈꢃïꢃꢍꢊꢂƒ)ꢃ²ꢃ6XSSO\ꢃ'%ꢎ  
6XSSO\ꢃ'%ꢃ ꢃꢄꢈꢁꢇƒ)  
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Figure 71  
In response to the reduction in room sensible heat gain, the coil capacity is  
throttled, raising the supply air temperature from D to D’ to balance the new  
room sensible heat gain. This new supply air temperature is dictated by the  
equation:  
Sensible Heat Gain  
1.085 × (Room DB Supply DB)  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
Supply Airflow (cfm) =  
Since the supply airflow and the desired room dry-bulb temperature are  
constant, the only variable that responsed to this change in sensible heat gain is  
supply air temperature.  
47,000 Btu/hr  
1.085 × (78°F Supply DB)  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
= 3,430 cfm  
Supply DB = 65.4°F  
This new supply air temperature D’ is delivered in sufficient quantity to absorb  
the room’s sensible heat gain, but it does not fall on the part-load SHR line and  
is not dry enough to completely absorb the latent heat gain. When the  
conditioned air enters the room, it mixes with room air along the 0.70 sensible  
heat ratio line from D’ to A’. The resulting room condition A’, where the SHR  
line intersects the room dry-bulb temperature line (78°F), shows that the  
relative humidity increased to 61%.  
44  
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period six  
Psychrometric Analyses  
notes  
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2$  
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Figure 72  
This is the manner in which a constant-volume, variable-temperature system  
with a modulating coil performs. It provides a constant quantity of air to the  
room and responds to part-load conditions by varying the supply air  
temperature. This is performed by modulating the flow of the cooling fluid  
through the coil, typically using a two-way or three-way control valve controlled  
by a thermostat that senses the room dry-bulb temperature. Such a system can  
provide good dry-bulb temperature control. As the sensible heat ratio changes  
from full load, however, it may lose control of the room relative humidity.  
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Figure 73  
One method of improving the constant-volume system’s ability to control room  
humidity is to reheat the supply air. In this example, reheat is provided by a  
heating coil located downstream of the air handler. This reheat coil is controlled  
by a thermostat sensing the room dry-bulb temperature, while the cooling coil  
is controlled to provide a constant leaving-air temperature.  
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period six  
Psychrometric Analyses  
notes  
(IIHFWꢀRIꢀ$GGLQJꢀ5HKHDW  
ꢇꢊꢆꢀꢀꢀꢃ%WXꢋKU  
 ꢃꢅꢆꢇꢅꢀꢃFIP  
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6XSSO\ꢃ'%ꢃ ꢃꢄꢈꢁꢇƒ)  
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Figure 74  
Using the part-load conditions from the previous example, the room’s sensible  
heat gain is reduced from 80,000 Btu/hr to 47,000 Btu/hr while the latent heat  
gain remains the same.  
Sensing the reduction in dry-bulb temperature due to the lower sensible heat  
gain, the room thermostat assumes control of the reheat coil. The cooling coil is  
controlled to provide a constant supply air temperature  
(D = 56.5°F DB), while the reheat coil is controlled to add just enough heat to  
the supply air to offset the reduction in room sensible-heat gain.  
Since the supply airflow is constant and the desired room dry-bulb temperature  
and sensible heat gain are known, we can calculate the required “re-heated”  
supply air temperature.  
47,000 Btu/hr  
1.085 × (78°F Supply DB)  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
= 3,430 cfm  
Supply DB = 65.4°F  
Since the supply air leaving the coil is sensibly heated (i.e., no moisture is  
added or removed), it moves horizontally along a constant humidity-ratio line  
from D to E. The resulting supply air conditions are 65.4°F DB, 58.9°F WB.  
46  
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period six  
Psychrometric Analyses  
notes  
(IIHFWꢀRIꢀ$GGLQJꢀ5HKHDW  
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Figure 75  
This supply air mixes with room air along the part-load 0.70 SHR line from E to  
A, arriving at the desired room conditions A. Now, if the room’s latent heat gain  
were also changed, the resulting room conditions would not fall exactly on A,  
but on the appropriate SHR line that runs through E.  
Adding reheat permits better room humidity control at various part-load  
conditions while maintaining room dry-bulb temperature control. Realize,  
however, that this system uses more energy than the previous constant-volume  
system with a modulating cooling coil: it constantly cools the supply air to  
56.5°F, then reheats the air as necessary when the building sensible load drops.  
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Figure 76  
Another method of improving the constant-volume system's ability to control  
room humidity is to bypass mixed air around the cooling coil. In this example,  
face-and-bypass dampers are placed in front of the cooling coil and used to  
vary the portion of the supply air that actually passes through the coil, thus  
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period six  
Psychrometric Analyses  
varying the supply air temperature as the two airstreams mix downstream of  
the air handler.  
notes  
The face-and-bypass dampers are controlled by the room dry-bulb thermostat.  
The cooling coil is allowed to “run wild,” causing the air that does pass through  
it to be cooled more at partial airflows.  
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Figure 77  
At our example part-load conditions, the room thermostat assumes control of  
the face-and-bypass dampers, which reduces the amount of air passing  
through the cooling coil. Since the coil is now “running wild,” the reduced  
airflow through the coil (1,870 cfm) is cooled and dehumidified more than at full  
load (D). When the conditioned air mixes with the bypass air (1,560 cfm), the  
required supply air condition (3,430 cfm at E) results.  
48  
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period six  
Psychrometric Analyses  
notes  
(IIHFWꢀRIꢀ0L[HGꢁ$LUꢀ%\SDVV  
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Figure 78  
This supply air E mixes with room air along the part-load 0.70 SHR line, arriving  
at the resulting new room conditions A’. While the quantity and temperature of  
supply air are suitable to absorb the room’s sensible heat gain, they are unable  
to completely absorb the latent heat gain. The result is a shift in room  
conditions from the design point A to 78°F DB, 58% RH (A’).  
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Figure 79  
The final method of part-load control we will analyze is to vary the supply  
airflow to the room.  
Let’s look at the same example again, this time using a simple variable-air-  
volume (VAV) system. This system responds to part-load conditions by  
supplying a variable quantity of constant-temperature air. At full load, this  
system looks the same on the psychrometric chart as the constant-volume  
system—it supplies 3,430 cfm of 56.5°F air to the room.  
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period six  
Psychrometric Analyses  
notes  
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Figure 80  
At part load, when the SHR of the room is reduced from 0.80 to 0.70, the VAV  
system responds by reducing the quantity of 56.5°F air supplied to the room to  
match the reduced sensible heat gain. The part-load sensible heat gain of  
47,000 Btu/hr and the constant supply air temperature, 56.5°F DB, are used to  
determine the required part-load air quantity.  
47,000 Btu/hr  
1.085 × (78°F 56.5°F)  
ꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀꢀ  
Supply Airflow (cfm) =  
= 2,015 cfm  
When the conditioned supply air D enters the room, it mixes with room air  
along the part load SHR line from D to A’. This quantity and temperature of  
supply air are suitable to absorb the room's sensible heat gain, but are unable  
to completely absorb the latent heat gain. The result is a shift in the room  
conditions from the design point A to 78°F DB and 59% RH (A’). While the  
simple VAV system does a better job of controlling room humidity than the  
simple constant-volume system, it is still unable to maintain the desired  
condition of 50% RH.  
To more accurately determine the final room conditions, you would cycle  
through the psychrometric chart again. First, use the new room condition A’ to  
calculate the mixed-air entering conditions. Then use the coil curves to find the  
condition of the 56.5°F dry-bulb supply air. Finally, draw the SHR line through  
this new supply air condition to find the resulting room conditions. Repeating  
this process a few times allows the room condition to converge and be equal to  
the condition used in the previous iteration.  
50  
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period six  
Psychrometric Analyses  
notes  
6RIWZDUHꢀ7RROV  
Figure 81  
The psychrometric chart is a visual tool that helps designers find solutions to  
many common HVAC problems by plotting conditions on the chart.  
Today, many of these same problems can be quickly solved by computers,  
which can often eliminate the need for a graphical solution altogether. Still, a  
basic understanding of psychrometric principles is required to use these tools,  
and is fundamental to the science of air conditioning.  
Instead of relying solely on the “typical” coil curves printed on the  
psychrometric chart, many manufacturers provide computerized coil selection  
programs to determine the actual performance of specific coils. Software tools  
are also available to assist you in performing psychrometric calculations, such  
as determining the properties of air at a given set of conditions, and finding the  
conditions that result when two air streams are mixed.  
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period seven  
Review  
notes  
3V\FKURPHWU\  
SHULRGꢀVHYHQ  
5HYLHZ  
Figure 82  
Let’s review some of the main concepts from this clinic on psychrometry.  
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Figure 83  
'U\ꢀ%XOEꢂ7HPSHUDWXUHꢂꢅƒ)ꢆ  
The lines of the psychrometric chart represent five physical properties of air:  
dry bulb, wet bulb, dew point, humidity ratio, and relative humidity.  
If any two of these properties are known, the remaining properties can be  
determined from the chart.  
52  
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period seven  
Review  
notes  
'HWHUPLQLQJꢀ0L[HGꢁ$LUꢀ&RQGLWLRQV  
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Figure 84  
In Period Two, a method was discussed to determine the resulting properties of  
an air mixture. By plotting the conditions of the outdoor air and recirculated  
air, and using the percentage of outdoor air, the resulting condition of the air  
mixture was calculated and plotted on a straight line from A to B connecting  
the two air conditions.  
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Figure 85  
In Period Three, the ratio of sensible heat gain to total heat gain was  
discussed. With the aid of the sensible heat ratio scale on the chart, an SHR line  
was drawn. It was also shown that any combination of air conditions that fall on  
this line will maintain the desired room conditions A. Each set of conditions  
requires a different supply airflow.  
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period seven  
Review  
notes  
'HWHUPLQLQJꢀ&RLOꢀ/HDYLQJꢀ&RQGLWLRQV  
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Figure 86  
After determining the entering air conditions for the coil and the slope of the  
SHR line, the coil curves were used to find the required supply air conditions.  
This point (D) was established by the intersection of the coil curve and the SHR  
line.  
By knowing the design room conditions A and the required supply air  
conditions D, the corresponding supply airflow could be calculated.  
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Figure 87  
After the entering (C) and leaving (D) coil conditions were established, the  
enthalpies for each were read from the psychrometric chart. These enthalpy  
values and the previously calculated supply airflow were used to determine the  
refrigeration load in Btu/hr or tons.  
54  
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period seven  
Review  
notes  
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Figure 88  
The resulting psychrometric chart plot represents the changes that a volume of  
air undergoes as it travels through a typical air conditioning system.  
In this illustration, recirculated air A is mixed with outdoor air B, producing a  
mixed air condition C.  
This air mixture passes through the cooling and dehumidifying coil, with the  
changes in dry-bulb temperature and humidity ratio represented by the coil  
curve from C to D.  
This supply air D enters the room and mixes with the room air along the SHR  
line from D to A, absorbing the room’s sensible and latent heat gains, to  
maintain the room at desired conditions A.  
Again, for this specific supply air condition, a specific airflow is required to  
maintain the desired room conditions.  
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period seven  
Review  
notes  
Figure 89  
For more information, refer to the following references:  
Trane Air Conditioning Manual  
ASHRAE Handbook—Fundamentals  
Fundamentals of Thermodynamics and Psychrometrics, ASHRAE self-  
directed learning course  
Psychrometrics: Theory and Practice, ASHRAE  
For information on additional educational materials available from Trane,  
contact your local Trane sales office (request a copy of the Educational  
Materials price sheet—Trane order number EM-ADV1) or visit our online  
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Quiz  
Questions for Period 1  
1
2
3
4
5
Given air conditions of 80°F DB and 60% RH, find the humidity ratio and  
dew-point temperature.  
Given air conditions of 85°F DB and a humidity ratio of 90 grains/lb, find the  
relative humidity and wet-bulb temperature.  
Given air conditions of 74°F WB and 60% RH, find the dry-bulb temperature  
and humidity ratio.  
Given air conditions of 80°F DB and a humidity ratio of 64 grains/lb, find the  
relative humidity and wet-bulb temperature.  
Given air conditions of 90°F DB and 68°F WB, find the dew-point  
temperature and relative humidity.  
Questions for Period 2  
6
Given outdoor air conditions of 95°F DB, 78°F WB; indoor design conditions  
of 80°F DB, 67°F WB; total airflow of 20,000 cfm; and outdoor airflow of  
4,000 cfm:  
a
b
c
Find the dry-bulb temperature of the mixture.  
Plot all three conditions on the psychrometric chart.  
Find the wet-bulb temperature of the mixture.  
7
Given outdoor air conditions of 90°F DB, 80°F WB; indoor design conditions  
of 78°F DB, 65°F WB; total airflow of 40,000 cfm; and outdoor airflow of  
6,000 cfm:  
a
b
c
Find the dry-bulb temperature of the mixture.  
Plot all three conditions on the psychrometric chart.  
Find the wet-bulb temperature of the mixture.  
Questions for Period 3  
8
Given a sensible heat ratio of 0.80 and indoor design conditions of 78°F DB  
and 66°F WB:  
a
b
Draw the SHR line on the psychrometric chart.  
Find the dry-bulb and wet-bulb temperatures of the air where this SHR  
line crosses the 90% RH curve.  
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Quiz  
Questions for Period 4  
9
Given a room with a 42,000 Btu/hr sensible heat gain and a 56,000 Btu/hr  
total heat gain (excluding ventilation heat gain); and indoor design  
conditions of 80°F DB and 50% RH:  
a
b
Determine the sensible heat ratio.  
Draw the SHR line.  
10 Given a room with an 80,000 Btu/hr sensible heat gain, a 20,000 Btu/hr  
latent heat gain (excluding ventilation heat gain), and indoor design  
conditions of 80°F DB and 67°F WB, find the wet-bulb temperature of the  
supply air if it leaves the cooling coil at 60°F DB.  
Questions for Period 5  
11 Given indoor design conditions of 80°F DB and 67°F WB, if the air leaves  
the cooling coil at 57°F DB, find the airflow (in cfm) required to satisfy a  
1,000 Btu/hr sensible heat gain.  
12 Given that air enters the cooling coil at 85°F DB, 69°F WB and leaves at 58°F  
DB, 56.4°F WB, if the supply airflow is 7,000 cfm, find the total refrigeration  
load, in tons.  
13 Given indoor design conditions of 78°F DB, 65°F WB; outdoor conditions of  
95°F DB, 75°F WB; a sensible heat gain of 156,000 Btu/hr; a latent heat gain  
of 39,000 Btu/hr; and 25% outdoor air:  
a
Plot the indoor and outdoor design conditions on the psychrometric  
chart.  
b
c
d
e
f
Find the mixed-air conditions entering the cooling coil.  
Draw the SHR line.  
Draw the coil curve and determine the coil leaving-air conditions.  
Calculate the supply airflow.  
Determine the enthalpy difference between the entering- and leaving-  
air conditions.  
g
Calculate the refrigeration load in tons.  
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Answers  
1
2
3
4
5
93 grains/lb, 64.8°F DP  
49.5% RH, 70.5°F WB  
85°F DB, 110 grains/lb  
41% RH, 64°F WB  
56°F DP, 32% RH  
6 a  
4,000 cfm  
20,000 cfm  
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= 0.20  
95°F × 0.20 = 19°F  
80°F × 0.80 = 64°F  
Mixed-Air Temperature = 19°F + 64°F = 83°F  
b
See Figure 90.  
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Figure 90  
c
69.4°F WB  
7 a  
6,000 cfm  
40,000 cfm  
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= 0.15  
95°F × 0.15 = 13.5°F  
78°F × 0.85 = 66.3°F  
Mixed-Air Temperature = 13.5°F + 66.3°F = 79.8°F  
b
c
See Figure 91.  
67.4°F WB (See Figure 91.)  
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Answers  
ꢏꢉꢎꢋƒ)  
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Figure 91  
8 a The SHR line crosses the saturation curve at 56°F WB (See Figure 92.)  
b
60°F DB, 58°F WB (See Figure 92.)  
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Figure 92  
9 a  
b
42,000 Btu/hr  
56,000 Btu/hr  
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SHR =  
= 0.75  
See Figure 93.  
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Answers  
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Figure 93  
10  
80,000 Btu/hr  
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SHR =  
= 0.80  
80,000 Btu/hr + 20,000 Btu/hr  
58.3°F WB (See Figure 94.)  
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Figure 94  
11  
1,000 Btu/hr  
1.085 × (80°F 57°F)  
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Supply Airflow (cfm) =  
= 40 cfm  
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Answers  
12 See Figure 95.  
Refrigeration Load = 4.5 × 7,000 cfm × (33.2 24.2) = 283,500 Btu/hr  
283,500 Btu/hr  
12,000 Btu/hr/ton  
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= 23.6 tons of refrigeration  
Figure 95  
13 a See Figure 96.  
b
95°F × 0.25 = 23.75°F  
78°F × 0.75 = 58.50°F  
Mixed-Air Temperature = 23.75°F + 58.50°F = 82.25°F  
Mixed-Air Conditions = 82.25°F DB, 67.7°F WB (See Figure 96.)  
c
d
156,000 Btu/hr  
156,000 Btu/hr + 39,000 Btu/hr  
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SHR =  
= 0.80 (See Figure 96.)  
Leaving-Coil Conditions = 57°F DB, 54.4°F WB (See Figure 96.)  
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Figure 96  
e
156,000 Btu/hr  
1.085 × (78°F 57°F)  
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Airflow (cfm) =  
= 6,847 cfm  
f
h1 h2 = 32.1 23.7 = 8.4 Btu/lb  
g
Refrigeration Load = 4.5 × 6,847 cfm × 8.4 Btu/lb = 258,817 Btu/hr  
258,817 Btu/hr  
12,000 Btu/hr/ton  
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= 21.6 tons  
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Glossary  
ASHRAE American Society of Heating, Refrigerating and Air-Conditioning  
Engineers  
coil curves These represent the changes in dry-bulb and wet-bulb  
temperatures as air passes through a “typical” cooling coil.  
constant-volume system A type of air-conditioning system that varies the  
temperature of a constant volume of air supplied to meet the changing load  
conditions of the space.  
dew-point temperature The temperature at which moisture leaves the air and  
condenses on surfaces.  
dry-bulb temperature A measure of the amount of sensible heat in the air.  
enthalpy A quantity that describes the total amount of heat energy, both  
sensible and latent, in one pound of air at a given condition.  
humidity ratio A quantity that describes the actual weight of the water in an  
air – water vapor mixture.  
interior space A conditioned space that is surrounded by other conditioned  
spaces, with no perimeter walls or windows. It typically requires some degree  
of cooling all year long to overcome the heat generated by people, lighting, etc.  
latent heat Heat that causes a change in the air’s moisture content with no  
change in dry-bulb temperature.  
mixed-air bypass A method of part-load control that uses face-and-bypass  
dampers, located in front of the cooling coil, to vary the portion of the supply air  
that passes through the coil. This varies the supply air temperature as the two  
airstreams mix downstream of the coil.  
outdoor air Air brought in to the building, either by a ventilation system or  
through openings provided for natural ventilation, from outside the building.  
psychrometric chart A tool used to graphically display the properties of air.  
psychrometry The science dealing with the physical laws of air – water  
mixtures.  
recirculated return air Air removed from the conditioned space and reused as  
supply air, usually after passing through an air-cleaning and -conditioning  
system, for delivery to the conditioned space.  
relative humidity A comparison of the amount of moisture that a given  
amount of air is holding, to the amount of moisture that the same amount of air  
can hold, at the same dry-bulb temperature.  
return air Air that is removed from the conditioned space(s) and either  
recirculated or exhausted.  
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Glossary  
saturation curve This represents the moisture content that constitutes  
complete saturation of air at the various dry-bulb temperatures.  
saturation point The maximum amount of water vapor that one pound of dry  
air can hold at a given dry-bulb temperature.  
sensible heat Heat that causes a change in the air’s dry-bulb temperature with  
no change in moisture content.  
sensible heat ratio (SHR) The ratio of sensible heat gain to total (sensible +  
latent) heat gain.  
specific volume The volume of one pound of dry air at a specific temperature  
and pressure.  
supply air Air that is delivered to the conditioned space by mechanical means  
for ventilation, heating, cooling, humidification, or dehumidification.  
supply duct system A system that transports the primary air from the central  
air handler to the VAV terminal units and then on to the space diffusers.  
ton of refrigeration A quantity that is equal to 12,000 Btu/hr.  
variable-air-volume (VAV) system A type of air-conditioning system that  
varies the volume of constant temperature air supplied to meet the changing  
load conditions of the space.  
wet-bulb temperature A measure of the dryness of the air, obtained by using  
a thermometer with a bulb that is covered by a wet wick.  
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Literature Order Number  
File Number  
TRG-TRC001-EN  
E/AV-FND-TRG-TRC001-1099-EN  
ED-FND-TRG-TRC001-199-EN  
Inland-La Crosse  
The Trane Company  
Supersedes  
Worldwide Applied Systems Group  
3600 Pammel Creek Road  
La Crosse, WI 54601-7599  
Stocking Location  
An American Standard Company  
Since The Trane Company has a policy of continuous product improvement, it reserves the right to change  
design and specifications without notice.  
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