presented by eugene silberstein, m.s., cmhe, beap suffolk county community college cengage learning...

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Presented by Eugene Silberstein, M.S., CMHE, BEAP Suffolk County Community College Cengage Learning HVAC EXCELLENCE EDUCATORS CONFERENCE SOUTH POINT HOTEL & CASINO MARCH 31 – APRIL 2, 2014

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Presented by

Eugene Silberstein, M.S., CMHE, BEAP

Suffolk County Community College

Cengage Learning

HVAC EXCELLENCE EDUCATORS CONFERENCE

SOUTH POINT HOTEL & CASINO

MARCH 31 – APRIL 2, 2014

If we change the way we look at things, the things

we look at change

IXS

Chocolate Pudding

1 x 1 x 72

1 x 2 x 36

1 x 3 x 24

1 x 4 x 18

1 x 6 x 12

1 x 8 x 9

2 x 2 x 18

2 x 3 x 12

2 x 4 x 9

2 x 6 x 6

3 x 4 x 6

3 x 3 x 8

743928231918

221715141314

Pressure

Heat Content

(psia)

Btu/lb

LINES OF CONSTANT PRESSURELINES OF CONSTANT ENTHALPY

HEAT CONTENT INCREASES

HEAT CONTENT DECREASES

PRESSURE RISES

PRESSURE DROPS

Pressure

Heat Content

(psia)

Btu/lbBtu/lb

SATURATION CURVE

THE SATURATION CURVE

• Under the curve, the refrigerant follows the pressure-temperature relationship

• The left side of the saturation curve represents 100% liquid

• The right side of the saturation curve represents 100% vapor

• For non-blended refrigerants, one pressure corresponds to one temperature

Pressure

Heat Content

(psia)

Btu/lb

LINES OF CONSTANT TEMPERATURE

Pressure

Heat Content

(psia)

Btu/lb

LINES OF CONSTANT VOLUME (ft3/lb)

Pressure

Heat Content

(psia)

Btu/lb

LINES OF CONSTANT ENTROPY

Pressure

Heat Content

(psia)

Btu/lb

LINES OF CONSTANT QUALITY

Pressure

Heat Content

(psia)

Btu/lb

PUT IT ALL TOGETHER…

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

12 20 25 31 35 8 8 8 8 8 9 9 9 9 9 1 1 1 1 1

24

36

52

72

99

132

172

221

0 2 4 6 8 0 2 4 6 8 0 0 0 0 0

0 2 4 6 8Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-12 (Simplified)

160°F

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

15 24 31 40 46

39

58

84

117

159

211

275

352

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

160°F

110

112

123

119

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

13 28 45

63

93

133

186

251

334

434

557

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-410A (Simplified)

160°F

123 133 143 140 21 37 53

148 152

REPEATING vs. NON-REPEATING CYCLES

High Pressure High Temperature

High Pressure High Temperature

Low Pressure Low Temperature

Low Pressure Low Temperature

Liquid

Liquid

Vapor

Vapor

COMPRESSOR

CONDENSER

METERING DEVICE

EVAPORATOR

COMPRESSOR

CONDENSER

METERING DEVICE

EVAPORATOR

Superheated VaporSubcooled Liquid Saturated Refrigerant

Superheated Region

Saturated Region

Subcooled Region

Pressure

Heat Content

Pressure

Heat Content

Pressure

Heat Content

(psia)

Btu/lb

Saturation

Height Above Saturation

VAPORLIQUID

Saturation

Distance Below Saturation

VAPORLIQUID

Pressure

Heat Content

(psia)

Btu/lb

Pressure

Heat Content

(psia)

Btu/lb

PUT IT ALL TOGETHER…

A

B C D

E

Pressure

Heat Content

(psia)

Btu/lb

PUT IT ALL TOGETHER…

A

B C D

EA

B C D

E

E to A: CONDENSER (Including discharge and liquid line)

A to B: METERING DEVICE

B to C: EVAPORATOR

C to D: SUCTION LINE

D to E: COMPRESSOR

A

B C D

E

NET REFRIGERATION EFFECT

The portion of the system that provides the desired cooling or conditioning of the space or products being

treated.

NET REFRIGERATION EFFECT

• The larger the NRE, the greater the heat transfer rate per pound of refrigerant circulated

• NRE is in the units of btu/lb

• Cooling effect can be increased by increasing the NRE or by increasing the mass flow rate

• The cooling effect can be decreased by decreasing the NRE or by decreasing the rate of refrigerant circulation through the system

NRE Example

• Heat Content at point B = 35 btu/lb

• Heat Content at point C = 85 btu/lb

• NRE = C – B = 85 btu/lb – 35 btu/lb

NRE = 50 btu/lb

• Each pound of refrigerant can therefore hold 50 btu of heat energy

• How many btu does it take to make 1 ton?

How Many btu = 1 Ton?• 12,000 btu/hour = 1 Ton = 200 btu/min

• From the previous example, how many lb/min do we have to move through the system to get 1 ton?

• 200 btu/min/ton ÷ 50 btu/lb = 4 lb/min

• We must circulate 4 pounds of refrigerant through the system every minute to obtain one ton of refrigeration

• Mass Flow Rate Per Ton

NRE and MFR/ton• The NRE determines the number of btu that a

pound of refrigerant can hold

• The larger the NRE the more btu can be held by the pound of refrigerant

• As the NRE increases, the MFR/ton decreases

• As the NRE decreases, the MFR/ton increases

• NRE = Heat content at C – Heat content at B

• MFR/ton = 200 ÷ NRE

• Cool, huh?

A

B C D

E

THE SUCTION LINE

The line that connects the outlet of the evaporator to the inlet of the compressor. This line is field installed

on split-type air conditioning systems.

SUCTION LINE • The suction line should be as short as possible

• The amount of heat introduced to the system through the suction line should be minimized

• Damaged suction line insulation increases the amount of heat added to the system and decreases the system’s operating efficiency

• Never remove suction line insulation without replacing

• Seal the point where insulation sections meet

A

B C D

E

D

E

A

B C D

E

HEAT OF WORK

The quantity, in btu/lb that represents the amount of heat that is added to the refrigerant during the

compression process.

HEAT OF WORK (HOW)• The HOW indicates the amount of heat added

to a pound of refrigerant during compression

• As the pressure of the refrigerant increases, the heat content of the refrigerant increases as well

• Heat gets concentrated in the compressor

• As HOW increases, efficiency decreases

• As HOW decreases, system efficiency increases

• HOW = Heat content at E – Heat content at D

A

B C D

E

HEAT OF COMPRESSION

The quantity, in btu/lb that represents the amount of heat that is added to the system, outside of the

evaporator

HEAT OF COMPRESSION (HOC)

• The HOW indicates the amount of heat added to a pound of refrigerant outside the evaporator

• Comprised of the HOW and the suction line

• As HOC increases, efficiency decreases

• As HOC decreases, system efficiency increases

• HOW = Heat content at E – Heat content at C

A

B C D

E

TOTAL HEAT OF REJECTION

The quantity, in btu/lb that represents the amount of heat that is removed from the system. THOR includes

the discharge line, condenser and liquid line.

TOTAL HEAT OF REJECTION (THOR)

• THOR indicates the total amount of heat rejected from a system

• Refrigerant (hot gas) desuperheats when it leaves the compressor (sensible heat transfer)

• Once the refrigerant has cooled down to the condensing temperature, a change of state begins to occur (latent heat transfer)

• After condensing, refrigerant subcools• THOR = Heat content at E – Heat content at A• THOR = NRE + HOC

SUBCOOLING & FLASH GAS

• Subcooling is a good thing, right?

• Flash gas is a good thing, right?

• Are flash gas and subcooling related?

• How can we tell?

• Stay tuned...

A

B C D

E

HIGH SUBCOOLING....

(Only a slight Exaggeration)

What happened to the amount of flash gas?

A

B C D

E

LARGE AMOUNT OF FLASH GAS....

(Only a slight Exaggeration)

What happened to the subcooling?

SUBCOOLING & FLASH GAS

• Subcooling and flash gas are inversely related to each other

• As the amount of subcooling increases, the percentage of flash gas decreases

• As the percentage of flash gas increases, the amount of subcooling decreases

A

B C D

E

COMPRESSION RATIO

Determined by dividing the high side pressure (psia) by the low side pressure (psia)

High-side pressure

Low-side pressure

COMPRESSION RATIO

• Represents the ratio of the high side pressure to the low side pressure

• Directly related to the amount of work done by the compressor to accomplish the compression process

• The larger the compression ratio, the larger the HOW and HOC and the lower the system MFR

• The larger the HOW and HOC, the lower the system efficiency

• Absolute pressures must be used

ABSOLUTE PRESSURE

• Absolute pressure = Gauge pressure + 14.7

• Round off to 15, for ease of calculation

• Example 1– High side pressure (psig) = 225 psig– High side pressure (psia) = 225 + 15 = 240 psia– Low side pressure (psig) = 65 psig– Low side pressure (psia) = 65 + 15 = 80 psia– Compression ratio = 240 psia ÷ 80 psia = 3:1

Low Side Pressure in a Vacuum?

• First, convert the low side vacuum pressure in inches of mercury to psia

• Use the following formula

(30” Hg – vacuum reading) ÷ 2

• Example– High side pressure = 245 psig– High side pressure (psia) = 245 + 15 = 260 psia– Low side pressure = 4”Hg– Low side (psia) = (30”hg – 4”Hg) ÷ 2 = 13 psia– Compression ratio = 260 ÷ 13 = 20:1

Meet Tammy…

2nd Floor

90th Floor

2 Lawyers + 1 Tammy = Wasted Time

Tammy’s 8-Hour Day• 9am – 10 am Work on 2nd Floor

• 10am – 11am Walk up

• 11am – 12 noon Work on 90th Floor

• 12 noon – 1pmWalk down

• 1 pm – 2pm Lunch

• 2pm – 3 pm Work on 2nd Floor

• 3 pm – 4 pm Walk up

• 4pm – 5 pm Work on 90th Floor

Hmmmmmmmmmmmm

• What if the law firm moves its 90th floor office to the 3rd floor?

• How will this affect Tammy’s productivity?

• Will she do more work? Less?

• What the heck does this have to do with air conditioning?

• How many licks does it take to get to the chocolaty center of a Tootsie Pop?

If Tammy’s office moves from the 90th floor to the 3rd floor, we

get something like this….

Tammy’s 8-Hour Day• 9:00 am – 10:00 am Work on 2nd Floor • 10:00 am – 10:05 am Walk up to 3rd Floor• 10:05 am – 11:05 noon Work on 3rd Floor• 11:05 am – 11:10 am Walk down to 2nd Floor• 11:10 am – 12:10 pm Work on 2nd Floor• 12:10 pm – 1:10 pm Lunch• 1:10 pm – 1:15 pm Walk up to 3rd Floor• 1:15 pm – 2:15 pm Work on 3rd Floor• 2:15 pm – 2:20 pm Walk down to 2nd Floor• 2:20 pm – 3:20 pm Work on 2nd Floor• 3:20 pm – 3:25 pm Walk up to 3rd Floor• 3:25 pm – 4:25 pm Work on 3rd Floor• 4:25 pm – 4:30 pm Walk down to 2nd Floor• 4:30 pm – 5:00 pm Work on 2nd Floor

Office Comparison

• 2nd Floor 90th Floor– 4 hours of work– 3 hours of walking up

and down the stairs– 1 hour lunch– Day ends on the 90th

Floor

• 2nd Floor 3rd Floor– 6 ½ hours of work– 30 minutes of walking

up and down the stairs– 1 hour lunch– Day ends on the 2nd

Floor

Which is better?

COMPRESSION RATIO

• Lower compression ratios higher system efficiency

• Higher compression ratios lower system efficiency

• The closer the head pressure is to the suction pressure, the higher the system efficiency, all other things being equal and operational

Causes of High Compression Ratio (High Side Issues)

• Dirty or blocked condenser coil

• Recirculating air through the condenser coil

• Defective condenser fan motor

• Defective condenser fan motor blade

• Defective wiring at the condenser fan motor

• Defective motor starting components (capacitor) at the condenser fan motor

Causes of High Compression Ratio (Low Side Issues)

• Dirty or blocked evaporator coil• Dirty air filter• Defective evaporator fan motor• Dirty blower wheel (squirrel cage)• Defective wiring at the evaporator fan motor• Closed supply registers• Blocked return grill• Loose duct liner• Belt/pulley issues

THEORETICAL HORSEPOWER PER TON

• Determines how much compressor horsepower is required to obtain 1 ton of cooling

• The ft-lb is a unit of work

• The ft-lb/min is a unit of power

• 33,000 ft-lb/min = 1 Horsepower

• The conversion factor between work and heat is 778 ft-lb/btu

• 33,000 ft-lb/min/hp ÷ 778 ft-lb/btu =

42.42 btu/min/hp

THEORETICAL HORSEPOWER PER TON

• THp/ton = (MFR/ton x HOW) ÷ 42.42• For example, if we had a system that had an

NRE of 50 and a HOW of 10, the THp/ton would be:

THp/ton = (200/NRE) x HOW ÷ 42.42THp/ton = (200/50) x 10 ÷ 42.42THp/ton = 4 x 10 ÷ 42.42

THp/ton = 40 ÷ 42.42THp/ton = 0.94

THp/ton Example

• If we had a 20-Hp reciprocating compressor and the THp/ton calculation yielded a result of 2 hp/ton, what would the expected cooling capability of the system be?

10 TONS16 TONS

5 TONS

25 TONS

3,492 TONS1 TON

3.8 TONS

20 TONS

What Affects the THp/ton Number?

• The Net Refrigeration Effect (NRE)

• The Heat of Work (HOW)

What Affects the NRE and HOW?

• Suction pressure

• Discharge pressure

• Compression Ratio

• Airflow through the coils

• Blowers and fans

• And so on, and so on, and so on, and so on….

Get the Picture?

MASS FLOW RATE OF THE SYSTEM• The amount of refrigerant that flows past any

given point in the system every minute

• Not to be confused with MFR/ton

• MFR/system is the actual refrigerant flow, while MFR/ton is the flow per ton

• MFR/system can be found by multiplying the MFR/ton by the number of tons of system capacity, or

MFR/system = (42.42 x Compressor HP) ÷ HOW

COOL STUFF• As the HOW increases, the MFR/system

decreases, and vice versa• As the Compression Ratio increases, the

HOW increases• As head pressure increases, or as suction

pressure decreases, the Compression Ratio increases

• As the MFR/system decreases, the capacity of the evaporator, condenser and compressor all decrease

• Let’s take a closer look…

EVAPORATOR CAPACITY• A function of the MFR/system and the NRE

• The MFR/system is in lb/min, the NRE is in btu/lb and the capacity of the evaporator is in btu/hour

Evaporator Capacity = MFR/system x NRE x 60

Btu Lb Btu 60 Min Hour Min Lb Hour

EVAPORATOR CAPACITY

• If the NRE or the MFR/system decreases, the evaporator capacity also decreases

• The “60” is a conversion factor from btu/min to btu/hour, given that there are 60 minutes in an hour

• Divide the evaporator capacity in btu/hour by 12,000 to obtain the evaporator capacity in tons

CONDENSER CAPACITY• A function of the MFR/system and the THOR

• The MFR/system is in lb/min, the THOR is in btu/lb and the capacity of the condenser is in btu/hour

Condenser Capacity = MFR/system x THOR x 60

Btu Lb Btu 60 Min Hour Min Lb Hour

COMPRESSOR CAPACITY• A function of the MFR/system and the

Specific volume of the refrigerant at the inlet of the compressor

• Calculated in cubic feet per minute, ft3/min

Compresser Capacity = MFR/system x Specific Volume

ft3 Lb ft3

Min Min Lb

COEFFICIENT OF PERFORMANCE (COP)

• The ratio of the NRE compared to the HOC

• If the HOC remains constant, any increases in NRE will increase the COP

• If the NRE remains constant, any decrease in HOC will increase the COP

• The COP is a contributing factor to the EER of an air conditioning system

• COP is a unitless value

COP EXAMPLE

• Heat content at point B = 35 btu/lb

• Heat content at point C = 104 btu/lb

• Heat content at point E = 127 btu/lb

• NRE = 104 btu/lb – 35 btu/lb = 69 btu/lb

• HOC = 127 btu/lb – 104 btu/lb = 23 btu/lb

• COP = 69 btu/lb ÷ 23 btu/lb = 3

• Notice that the “3” has no units

ENERGY EFFICIENCY RATIO (EER)

• A ratio of the amount of btus transferred to the amount of power used

• In the units of btu/watt• The conversion between btus and watts is

3.413• One watt of power generates 3.413 btu• For example, if a system required 50,000 btu of

heat, 14,650 watts of electric heat (14.65 kw) can be used

ENERGY EFFICIENCY RATIO (EER), Cont’d.

• The efficiency rating of an air conditioning system is the COP

• For each btu/lb introduced to the system in the suction line and the compressor, a number of btus equal to the NRE are absorbed into the system via the evaporator

• To convert the COP to energy usage, we multiply the COP by 3.413

EER EXAMPLE

• The NRE of a system is 70 btu/lb

• The HOC of the same system is 20 btu/lb

• The COP is 70 btu/lb ÷ 20 btu/lb = 3.5

• The EER = COP x 3.413

• EER = 3.5 x 3.413

• EER = 11.95

SEASONAL EER (SEER)

• Takes the entire conditioning system into account

• Varies depending on the geographic location of the equipment

• Ranges from 10% t0 30% higher than EER

• So, if the EER is 10, the SEER will range from 11 to 13

From the P-H Chart, We Can Find

• Compression Ratio• NRE• HOC• HOW• THOR• COP• MFR/ton

• THp/ton• MFR/system• Evaporator Capacity• Condenser Capacity• Compressor Capacity• EER of the System• SEER

Okay, Okay, Okay… How do I plot one of these things?

An R-22 A/C System…

• Condenser saturation temperature 120°F

• Condenser outlet temperature 100°F

• Evaporator saturation temperature 40°F

• Evaporator outlet temperature 50°F

• Compressor inlet temperature 60°F

• Compressor Horsepower: 4 hp

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7A

B C

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7A

B C D

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7A

B C D

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7A

B C D

E

0°F

20°F

40°F

60°F

80°F

100°F

120°F

140°F

3 4 4 5 1 1 1 1 1

39

58

84

117

211

352

1 1 1 2 2 0 2 7 1 5

Enthalpy in btu/lb (Heat Content)

Pressure (psia)

Pressure-Enthalpy (p-h) Diagram for R-22 (Simplified)

180°F

160°F

-20°F

-40°F

275

159

25

2 0 6 3

0.7A

B C D

E

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

COMPRESSION RATIO

HIGH SIDE PRESSURE (psia)

LOW SIDE PRESSURE (psia)

COMPRESSION RATIO = 275 psia ÷ 84 psia = 3.27:1

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

HEAT OF WORK

HEAT OF WORK = 125 btu/lb – 112 btu/lb = 13 btu/lb

HEAT CONTENT AT “E” – HEAT CONTENT AT “D”

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

HEAT OF COMPRESSION

HEAT OF COMPRESSION= 125 btu/lb – 110 btu/lb = 15 btu/lb

HEAT CONTENT AT “E” – HEAT CONTENT AT “C”

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

NET REFRIGERATION EFFECT

NRE = 110 btu/lb – 40 btu/lb = 70 btu/lb

HEAT CONTENT AT “C” – HEAT CONTENT AT “B”

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

MASS FLOW RATE PER TON

MFR/ton = 200 ÷ NRE =200 ÷ 70 btu/lb = 2.86 lb/min/ton

200 ÷ NRE

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

TOTAL HEAT OF REJECTION

THOR = 125 btu/lb – 40 btu/lb = 85 btu/lb

HEAT CONTENT AT “E” – HEAT CONTENT AT “A”

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

THEORETICAL HORSEPOWER PER TON

THp/ton = 2.86 lb/min/ton x 13 btu/lb ÷ 42.42 = 0.88 Hp/ton

[MFR/ton x HOW] ÷ 42.42

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

COEFFICIENT OF PERFORMANCE

COP = 70 btu/lb ÷ 15 btu/lb = 4.67

NRE ÷ HOC

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

MASS FLOW RATE OF THE SYSTEM

MFR/system = [42.42 x 4] ÷ 13 btu/lb = 13.05 lb/min

[42.42 x Compressor HP] ÷ HOW

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

CAPACITY OF THE EVAPORATOR

CAP/evap = 70 btu/lb x 13.05 x 60 = 54,810 btu/hour

NRE x MFR/system x 60

CAP/evap = 54,810 btu/hour ÷ 12,000 btu/hour/ton = 4.57 tons

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

CAPACITY OF THE CONDENSER

CAP/cond = 85 btu/lb x 13.05 x 60 = 66,555 btu/hour

THOR x MFR/system x 60

CAP/cond = 66,555 btu/hour ÷ 12,000 btu/hour/ton = 5.55 tons

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

CAPACITY OF THE COMPRESSOR

CAP/comp = 13.05 x 0.7 = 9.13 ft3/min

MFR/system x Specific Volume

High: 275 psia

Low: 84 psia

“A”: 40 btu/lb

“B”: 40 btu/lb

“C”: 110 btu/lb

“D”: 112 btu/lb

“E”: 125 btu/lb

ENERGY EFFICIENCY RATIO

EER = 4.67 x 3.413 = 15.94

COP x 3.413

SEER (low end) = 1.1 x EER = 1.1 x 15.94 = 17.5

SEER (high end) = 1.3 x EER = 1.3 x 15.94 = 20.7

40 110 112 125

275 psia

84 psia

61 psia

100 111

Let’s See What Happened…

• CR = 3.27• HOW = 13• HOC = 15• NRE = 70• MFR/ton = 2.86 lb/min• THp/ton = 0.88• COP = 4.67• MFR/system = 13.05• CAP/evap = 66,555 btu• EER = 15.9

• CR = 4.5• HOW = 14• HOC = 25• NRE = 60• MFR/ton = 3.33 lb/min• THp/ton = 1.1• COP = 2.4• MFR/system = 12.12• CAP/evap = 43,632 btu• EER = 8.19

Properly Operating System• Heat Content “A” = 40 btu/lb• Heat Content “B” = 40 btu/lb• Heat Content “C” = 109 btu/lb• Heat Content “D” = 111 btu/lb• Heat Content “E” = 125 btu/lb• High side pressure = 267 psig• High side pressure = 282 psia• Low side pressure = 70 psig• Low side pressure = 85 psia• Compressor Hp = 2.5 Hp• Specific Volume = 0.7

• NRE = 69 btu/lb• HOW = 14 btu/lb• HOC = 16 btu/lb• THOR = 85 btu/lb• Comp. Ratio = 3.32• MFR/ton = 2.9 lb/min/ton• THp/ton = 0.96 Hp/ton• COP = 4.3• MFR/system = 7.58 lb/min• CAP/evap = 31,381 btuh• CAP/cond = 38,658 btuh• CAP/comp = 5.3 ft3/min• EER = 14.68• SEER = 16.15 – 19.1

A/B C D E

Clogged Cap Tube System• Heat Content “A” = 39 btu/lb• Heat Content “B” = 39 btu/lb• Heat Content “C” = 112 btu/lb• Heat Content “D” = 118 btu/lb• Heat Content “E” = 134 btu/lb• High side pressure = 226 psig• High side pressure = 241 psia• Low side pressure = 59 psig• Low side pressure = 74 psia• Compressor Hp = 2.5 Hp• Specific Volume = 0.9

• NRE = 73 btu/lb• HOW = 16 btu/lb• HOC = 22 btu/lb• THOR = 95 btu/lb• Comp. Ratio = 3.26• MFR/ton = 2.74 lb/min/ton• THp/ton = 1.03 Hp/ton• COP = 3.3• MFR/system = 6.63 lb/min• CAP/evap = 29,039 btuh• CAP/cond = 37,791 btuh• CAP/comp = 5.97 ft3/min• EER = 11.26• SEER = 12.39 – 14.64

A/B C D E

System Okay System Clogged Increase/Decrease

NRE 69 73 Increase

HOW 14 16 Increase

HOC 16 22 Increase

THOR 85 95 Increase

Comp. Ratio 3.32 3.26 Decrease

MFR/ton 2.9 2.74 Decrease

THp/ton 0.96 1.03 Increase

COP 4.3 3.3 Decrease

MFR/system 7.58 6.63 Decrease

CAP/evap 31,381 (2.62) 29,039 (2.42) Decrease

CAP/cond 38,658 (3.22) 37,791 (3.15) Decrease

CAP/comp 5.3 5.97 Increase

EER 14.68 11.26 Decrease

SEER 16.15 – 19.1 12.39 – 14.64 Decrease

Contact Information...

Eugene Silberstein

Suffolk County Community College

1001 Crooked Hill Road

Brentwood, NY 11717

(631) 851-6897

E-mail: [email protected]