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8/8/2019 The Viscosity of a Fluid is Its Resistance to Shear or Flow
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The viscosity of a fluid is its resistance to shear or flow, and is a measure of the fluidsadhesive/cohesive or frictional properties. This arises because of the internal molecular friction withinthe fluid producing the frictional drag effect. There are two related measures of fluid viscosity which areknown as dynamic and kinematic viscosity.
Dynamic viscosity is also termed "absolute viscosity" and is the tangential force per unit arearequired to move one horizontal plane with respect to the other at unit velocity when maintained a unit
distance apart by the fluid.
Centipoise(CPS)
Millipascal (mPas)
Poise(P)
Centistokes
(cSt)
Stokes(S)
Saybolt SecondsUniversal
(SSU)
1 0.01 1 0.01 31
2 0.02 2 0.02 34
4 0.04 4 0.04 38
7 0.07 7 0.07 47
10 0.1 10 0.1 60
15 0.15 15 0.15 80
20 0.2 20 0.2 100
25 0.24 25 0.24 130
30 0.3 30 0.3 160
40 0.4 40 0.4 210
50 0.5 50 0.5 260
60 0.6 60 0.6 320
70 0.7 70 0.7 370
80 0.8 80 0.8 430
90 0.9 90 0.9 480
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100 1 100 1 530
120 1.2 120 1.2 580
140 1.4 140 1.4 690
160 1.6 160 1.6 790
180 1.8 180 1.8 900
200 2 200 2 1000
220 2.2 220 2.2 1100
240 2.4 240 2.4 1200
260 2.6 260 2.6 1280
280 2.8 280 2.8 1380
300 3 300 3 1475
320 3.2 320 3.2 1530
340 3.4 340 3.4 1630
360 3.6 360 3.6 1730
380 3.8 380 3.8 1850
400 4 400 4 1950
420 4.2 420 4.2 2050
440 4.4 440 4.4 2160
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460 4.6 460 4.6 2270
480 4.8 480 4.8 2380
500 5 500 5 2480
550 5.5 550 5.5 2660
600 6 600 6 2900
700 7 700 7 3380
800 8 800 8 3880
900 9 900 9 4300
1000 10 1000 10 4600
1100 11 1100 11 5200
1200 12 1200 12 5620
1300 13 1300 13 6100
1400 14 1400 14 6480
1500 15 1500 15 7000
1600 16 1600 16 7500
1700 17 1700 17 8000
1800 18 1800 18 8500
1900 19 1900 19 9000
2000 20 2000 20 9400
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2100 21 2100 21 9850
2200 22 2200 22 10300
2300 23 2300 23 10750
2400 24 2400 24 11200
2500 25 2500 25 11600
3000 30 3000 30 14500
3500 35 3500 35 16500
4000 40 4000 40 18500
4500 45 4500 45 21000
5000 50 5000 50 23500
5500 55 5500 55 26000
6000 60 6000 60 28000
6500 65 6500 65 30000
7000 70 7000 70 32500
7500 75 7500 75 35000
8000 80 8000 80 37000
8500 85 8500 85 39500
9000 90 9000 90 41080
9500 95 9500 95 43000
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15000 150 15000 150 69400
20000 200 20000 200 92500
30000 300 30000 300 138500
40000 400 40000 400 185000
50000 500 50000 500 231000
60000 600 60000 600 277500
70000 700 70000 700 323500
80000 800 80000 800 370000
90000 900 90000 900 415500
100000 1000 100000 1000 462000
125000 1250 125000 1250 578000
150000 1500 150000 1500 694000
175000 1750 175000 1750 810000
200000 2000 200000 2000 925000
Note! The viscosities are based on materials with a specific gravity of one (1).
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The calculator below can be used to convert between some common pressure units
Value (use period as decimal point)
Pa (N/m2 ) bar atmosphere mm Hg mm H 2 O m H 2 O kg/cm2 pound
square feet (psf) pound square inches (psi) inches Hg inches H 2 O ft H 2 O
Pressure Converting Tables
The tables below can be used to convert between some common pressure units:
Multiply by
Convertfrom
Convert to
Pa (N/m2 ) bar atmosphere mm Hg mm H 2 O m H 2 O kg/cm2
Pa (N/m2 ) 1 10-5 9.87 10-6 0.0075 0.1 10-4 1.02 10-5
bar 105 1 0.987 745 1.0197 104 10.197 1.0197
atmospher e
1.01 105 1.013 1 759.9 10132 10.13 1.03
mm Hg 133.3 1.33 10-3 1.32 10-3 1 13.3 0.013 1.36 10-3
mm H 2 O 10 0.000097 9.87 10-5 0.075 1 0.001 1.02 10-4
m H 2 O 104 0.097 9.87 10-2 75 1000 1 0.102
kg/cm2 9.8 104 0.98 0.97 735 10000 10 1
pound square feet
47.8 4.78 10-4 4.72 10-4 0.36 4.78 4.78 10-3 4.88 10-4
pound square
inches (psi)6894.76 0.069 0.068 51.7 689.7 0.690 0.07
inches Hg 3377 0.0338 0.033 25.33 337.7 0.337 0.034
þÿ
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inches H 2 O 248.8 2.49 10-3 2.46 10-3 1.87 24.88 0.0249 0.0025
Multiply by
Convert from
Convert to
pound square feet pound square
inches (psi)inches Hg inches H 2 O
Pa (N/m2 ) 0.021 1.450326 10-4 2.96 10-4 4.02 10-3
bar 2090 14.50 29.61 402
atmosphere 2117.5 14.69 29.92 407
mm Hg 2.79 0.019 0.039 0.54
mm H 2 O 0.209 1.45 10-3 2.96 10-3 0.04
m H 2 O 209 1.45 2.96 40.2
kg/cm2 2049 14.21 29.03 394
pound square feet (psf)
1 0.0069 0.014 0.19
pound squareinches (psi)
144 1 2.04 27.7
inches Hg 70.6 0.49 1 13.57
inches H 2 O 5.2 0.036 0.074 1
Some other Pressure Units
1 Pa (N/m2 ) = 0.0000102 Atmosphere (metric)1 Pa (N/m2 ) = 0.0000099 Atmosphere (standard)1 Pa (N/m2 ) = 0.00001 Bar 1 Pa (N/m2 ) = 10 Barad
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pH can be viewed as an abbreviation for power of Hydrogen - or more completely, power of theconcentration of the Hydrogen ion.
The mathematical definition of pH is a bit less intuitive but in general more useful. It says that the pH isequal to to the negative logarithmic value of the Hydrogen ion (H+) concentration, or
pH = -log [H +
]
pH can alternatively be defined mathematically as the negative logarithmic value of theHydroxonium ion (H3O
+) concentration. Using the Bronsted-Lowry approach
pH = -log [H 3O+ ]
pH values are calculated in powers of 10. The hydrogen ion concentration of a solution with pH 1.0 is10 times larger than the hydrogen concentration in a solution with pH 2.0. The larger the hydrogen ionconcentration, the smaller the pH.
• when the pH is above 7 the solution is basic (alkaline)
• when the pH is below 7 the solution is acidic
In pure neutral water the concentration of hydrogen and hydroxide ions are both 10-7 equivalents per liter.
pHIon Concentration(gram equivalent
per liter)Type of Solution
0 1.0
Acid Solution- Hydrogen ions -
H+
1 0.1
2 0.01
3 0.001
4 0.0001
5 0.00001
6 0.000001
7 0.0000001 Neutral Solution
8 0.000001 Basic (alkaline)Solution
- Hydroxide ions -
9 0.00001
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OH-
10 0.0001
11 0.001
12 0.01
13 0.1
14 1.0
Some common Products and their pH Values
pH values in some common products:
Product pH
Battery Acid 0
HCl in stomach acid 1
Lemon juice, vinegar 2-3
Orange juice 3-4
Acid rain 4
Black coffee 5
Urine, salvia 6
Pure water 7
Sea water 8
Baking soda 9
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Ammonia solution 10-11
Soapy water 12
Bleach 13
Oven cleaner 13-14
Drain cleaner 14
Boiler Efficiency may be indicated by
• Combustion Efficiency - indicates a burners ability to burn fuel measured by unburned fuel
and excess air in the exhaust• Thermal Efficiency - indicates the heat exchangers effectiveness to transfer heat from thecombustion process to the water or steam in the boiler, exclusive radiation and convection losses
• Fuel to Fluid Efficiency - indicates the overall efficiency of the boiler inclusive thermalefficiency of the heat exchanger, radiation and convection losses - output divided by input.
Boiler Efficiency is in general indicated by either Thermal Efficiency or Fuel to Fluid Efficiencydepending the context.
Boiler Efficiency
Boiler Efficiency related to the boilers energy output to the boilers energy input can be expressed as:
Boiler efficiency (%) = heat exported by the fluid (water, steam ..) / heat provided by the fuel x 100 (1)
Heat Exported from the Boiler to the Fluid
If a fluid like water is used to export heat from the boiler, exported heat can be expressed as:
q = ( m / t ) c p dT (2)
where
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q = heat exported (kJ/s, kW)
m / t = mass flow (kg/s)
m = mass (kg)
t = time (s)
c p = specific heat capacity (kJ/kg oC)
dT = temperature difference between inlet and outlet of the boiler ( oC)
For a steam boiler the heat exported as evaporated water at the saturation temperature can beexpressed as:
q = ( m / t ) he (3)
where
m = mass flow of evaporated water (kg)
t = time (s)
he = evaporation energy in the steam at the saturation pressure the boiler is running (kJ/kg)
Heat Provided by Fuel
The energy provided by fuel may be expressed in two ways 'Gross' or 'Net' Calorific Value.
Gross Calorific Value
This is the theoretical total of the energy in the fuel. The gross calorific value of the fuel includes the
energy used for evaporating the water in the combustion process. The flue gases from boilers are ingeneral not condensed. The actual amount of heat available to the boiler plant is therefore reduced.
• Gross Calorific Values of some common Fuels
An accurate control of the air supply is essential to the boilers efficiency.
• to much air cools the furnace and carries away useful heat
• too little air and the combustion will be incomplete. Unburned fuel will be carried over andsmoke produced
Net calorific value
This is the calorific value of the fuel, excluding the energy in the water vapor discharged to the stackin the combustion process. The combustion process can be expressed as:
[C + H (fuel)] + [O2 + N 2 (Air)] -> (Combustion Process) -> [CO2 + H 2 O + N 2 (Heat)]
where
C = Carbon
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H = Hydrogen
O = Oxygen
N = Nitrogen
In general it is possible to use the approximation:
net calorific value = gross calorific value - 10%
The values in the table below can be used as an indication of required area and boiler combustionheat load.
Boiler Capacity Required Chimney Area
kW Btu/h cm2 in2
15 51000 115 18
23 78000 150 23
35 119000 200 31
46 157000 250 39
58 198000 300 47
70 239000 350 54
81 276000 400 62
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93 317000 450 70
104 355000 500 78
116 396000 550 85
Remember, always check local authorities before final design.
Stoichiometric or Theoretical Combustion is the ideal combustion process where fuel is burnedcompletely.
A complete combustion is a process burning all the carbon (C) to (CO2), all the hydrogen (H) to (H2O)and all the sulphur (S) to (SO2).
With unburned components in the exhaust gas, such as C, H2, CO, the combustion process isuncompleted and not stoichiometric .
The combustion process can be expressed as:
[C + H (fuel)] + [O2 + N 2 (Air)] -> (Combustion Process) -> [CO2 + H 2 O + N 2 (Heat)]
where
C = Carbon
H = Hydrogen
O = Oxygen
N = Nitrogen
To determine the excess air or excess fuel for a combustion system we starts with the stoichiometricair-fuel ratio. The stoichiometric ratio is the perfect ideal fuel ratio where the chemical mixingproportion is correct. When burned all fuel and air is consumed without any excess left over.
Process heating equipment are rarely run that way. "On-ratio" combustion used in boilers and hightemperature process furnaces usually incorporates a modest amount of excess air - about 10 to 20%more than what is needed to burn the fuel completely.
If an insufficient amount of air is supplied to the burner, unburned fuel, soot, smoke, and carbonmonoxide exhausts from the boiler - resulting in heat transfer surface fouling, pollution, lower combustion efficiency, flame instability and a potential for explosion.
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To avoid inefficient and unsafe conditions boilers normally operate at an excess air level. This excessair level also provides protection from insufficient oxygen conditions caused by variations in fuelcomposition and "operating slops" in the fuel-air control system. Typical values of excess air areindicated for various fuels in the table below.
• if air content is higher than the stoichiometric ratio - the mixture is said to be fuel-lean
•
if air content is less than the stoichiometric ratio - the mixture is fuel-rich
• Excess air of different fuels
Example - Stoichiometric Combustion of Methane - CH4
The most common oxidizer is air . The chemical equation for stoichiometric combustion of methane -CH4 - with air can be expressed as
CH 4 + 2(O2 + 3.76N 2 ) -> CO2 + 2H 2 O + 7.52N 2
If more air is supplied some of the air will not be involved in the reaction. The additional air is termedexcess air , but the term theoretical air may also be used. 200% theoretical air is 100% excess air.
The chemical equation for methane burned with 25% excess air can be expressed as
CH 4 + 1.25 x 2(O2 + 3.76 N 2 ) -> CO2 + 2H 2 O + 0.5O2 + 9.4N 2
Excess Air and O2 and CO2 in Flue Gas
Aproximate values for CO2 and O2 in the flue gas as result of excess air are estimated in the tablebelow:
Excess Air %
Carbon Dioxide - CO2 - in Flue Gas (% volume)Oxygen inFlue Gas
for all fuels(% volume)
NaturalGas
PropaneButane
Fuel OilBituminous
CoalAnthracite
Coal
0 12 14 15.5 18 20 0
20 10.5 12 13.5 15.5 16.5 3
40 9 10 12 13.5 14 5
60 8 9 10 12 12.5 7.5
80 7 8 9 11 11.5 9
100 6 6 8 9.5 10 10
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Chemical, physical and thermal properties of Propane - C 3H 8 :
Molecular Weight 44.097
Specific Gravity 1.52
Specific Volume (ft 3 /lb, m3 /kg ) 8.84, 0.552
Density of liquid at atmospheric pressure (lb/ft 3, kg/m3) 36.2, 580
Vapor pressure at 25oC ( psia, MN/m2 ) 135.7, 0.936
Absolute Viscosity (lbm /ft s, centipoises) 53.8 10-6, 0.080
Sound velocity in gas (m/s) 253
Specific Heat - c p - (Btu/lboF or cal/g oC, J/kgK ) 0.39, 1630
Specific Heat Ratio - c p /c v 1.2
Gas constant - R - (ft lb/lboR, J/kg oC ) 35.0, 188
Thermal Conductivity (Btu/hr ft oF, W/moC ) 0.010, 0.017
Boiling Point - saturation pressure 14.7 psia and 760 mmHg - (oF, oC )
-44, -42.2
Latent Heat of Evaporation at boiling point (Btu/lb, J/kg ) 184, 428000
Freezing or Melting Point at 1 atm (oF, oC ) -309.8, -189.9
Latent Heat of Fusion (Btu/lb, J/kg ) 19.1, 44400
Critical Temperature (oF, oC ) 205, 96
Critical Pressure ( psia, MN/m2 ) 618, 4.26
Critical Volume (ft 3 /lb, m3 /kg ) 0.073, 0.0045
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Flammable yes
Heat of combustion (Btu/ft 3, Btu/lb, kJ/kg ) 2450, 21660, 50340
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The diagrams below indicates the water circulation rates through hot-water generators in imperial andSI-units.
Water Circulation - Boiler Capacity in BHP - Temperature drop in degreesFahrenheit
• 1 gal (US)/min =6.30888x10 -5 m3 /s = 0.0227 m3 /h = 0.06309 dm3(liter)/s = 2.228x10 -3 ft 3 /s =0.1337 ft 3 /min = 0.8327 Imperial gal (UK)/min
• 1 hp (English horse power) = 745.7 W = 0.746 kW = 550 ft lb/s = 2,545 Btu/h
Water Circulation - Boiler Capacity in MBtu/h - Temperature drop indegrees Fahrenheit
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• 1 Btu/h = 0.293 W
Water Circulation - Boiler Capacity in kW - Temperature drop in degreesCelsius
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• 1 kW = 3,412 Btu/h = 1.341 British hp
In an electrical systems the conductors should not be sized with voltage drops exceeding 3%. For a
12V system the maximum voltage drop should be less than 12 (V) x 3% = 0.36 (V).
The table below can be used to determine the combination of maximum current through a 12V electrical wire, size (AWG) and length of cable.
American Wire Gauge (AWG)
Length Current (amps)
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(feet)
5 10 15 20 25 30 40 50 60 70
15 16 12 10 10 8 8 6 6 4 4
20 14 12 10 8 8 6 6 4 4 4
25 14 10 8 8 6 6 4 4 2 2
30 12 10 8 6 6 4 4 2 2 2
40 12 8 6 6 4 4 2 2 1 1/0
50 10 8 6 4 4 2 2 1 1/0 1/0
60 10 6 6 4 2 2 1 1/0 2/0 2/0
70 10 6 4 2 2 2 1/0 2/0 2/0 3/0
80 8 6 4 2 2 1 1/0 2/0 3/0 3/0
90 8 4 4 2 1 1/0 2/0 3/0 3/0 4/0
Note! Failure to use an adequate size may result in fire. Always secure a wire with a fuse.
• 1 ft (foot) = 0.3048 m
Wire Gauge Design Procedure
1. calculate the total length of the wire from the source to the device and back again2. determine the amount of current in the wire3. correct wire gauge is in the intersection of amps and feet
Note! The wire size is required for a 3% voltage drop in 12 Volt circuits. Oversize the wire if thevoltage drop is critical
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American Wire Gauge (AWG) is a U.S. standard set of wire conductor sizes. The "gauge" is related tothe diameter of the wire.
The AWG standard includes copper, aluminum and other wire materials. Typical household copper wiring is AWG number 12 or 14. Telephone wire is usually 22, 24, or 26. The higher the gaugenumber, the smaller the diameter and the thinner the wire.
The table below can be used to convert American Wire Gauge (AWG) to square mm cross sectionalarea.
American WireGauge(AWG)
Diameter (inches)
Diameter (mm)
Cross SectionalArea(mm2)
0000 0.46 11.68 107.16
000 0.4096 10.40 84.97
00 0.3648 9.27 67.40
0 0.3249 8.25 53.46
1 0.2893 7.35 42.39
2 0.2576 6.54 33.61
3 0.2294 5.83 26.65
4 0.2043 5.19 21.14
5 0.1819 4.62 16.76
6 0.162 4.11 13.29
7 0.1443 3.67 10.55
8 0.1285 3.26 8.36
9 0.1144 2.91 6.63
10 0.1019 2.59 5.26
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11 0.0907 2.30 4.17
12 0.0808 2.05 3.31
13 0.072 1.83 2.63
14 0.0641 1.63 2.08
15 0.0571 1.45 1.65
16 0.0508 1.29 1.31
17 0.0453 1.15 1.04
18 0.0403 1.02 0.82
19 0.0359 0.91 0.65
20 0.032 0.81 0.52
21 0.0285 0.72 0.41
22 0.0254 0.65 0.33
23 0.0226 0.57 0.26
24 0.0201 0.51 0.20
25 0.0179 0.45 0.16
26 0.0159 0.40 0.13
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All wiring and electrical connections should comply with the National Electrical Code (NEC) and withlocal codes and practices.
Wire Gage (AWG)
Transformer Distance from Motor to Transformer (feet)
hp kVA 100 150 200 300 500
1.5 3 10 8 8 6 4
2 3 10 8 8 8 4
3 5 8 8 8 4 2
5 7.5 6 4 4 2 0
7.5 10 6 4 3 1 0
• 1 ft (foot) = 0.3048 m
If undersized wire is used between the motor and the power source, the starting and load carryingcapabilities of the motor will be limited.
All wiring and electrical connections should comply with the National Electrical Code (NEC) and withlocal codes and practices.
Wire Gage (AWG)
Transformer Distance - Motor to Transformer (Feet)
HP Volts kVA 100 150 200 300 500
1.5 230 3 12 12 12 12 10
2 460 3 12 12 12 12 12
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3 230 3 12 12 12 10 8
2 460 3 12 12 12 12 12
3 230 5 12 10 10 8 6
3 460 5 12 12 12 12 10
5 230 7.5 10 8 8 6 4
5 460 7.5 12 12 12 10 8
7.5 230 10 8 6 6 4 2
7.5 460 10 12 12 12 10 8
10 230 15 6 4 4 4 1
10 460 15 12 12 12 10 8
15 230 20 4 4 4 2 0
15 460 20 12 10 10 8 6
20 230 1) 4 2 2 1 0
20 460 1) 10 8 8 6 4
25 230 1) 2 2 2 0 0
30 230 1) 2 1 1 0 0
30 460 1) 8 6 6 4 2
40 230 1) 1 0 0 0 0
50 230 1) 1 0 0 0 0
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50 460 1) 4 4 2 2 0
30 230 1) 1 0 0 0 0
60 460 1) 4 2 2 0 0
75 230 1) 0 0 0 0 0
75 460 1) 4 2 2 0 0
1) The local power company should be consulted
• 1 ft (foot) = 0.3048 m
If undersized wire is used between the motor and the power source, the starting and load carrying capabilities of the motor will be limited.
There are three primary categories of steam traps:
• mechanical
• thermostatic
• thermodynamic
Popular traps in these categories includes the inverted bucket steam trap, the float steam trap, thethermostatic steam trap and the thermodynamic disc steam trap.Which one is preferred depends onthe application.
A steam trap prime missions is to remove condensate and air preventing escape of live steam from thedistribution system. The steam trap must adapt to the application. A disc thermodynamic steam trapshould never be used together with a modulating heat exchanger - and a floating ball steam trap isoverkill for draining steam pipes.
The table below can be used as a short guide for the selection of steam traps:
Type of SteamTrap
OperationNormalFailureModeNo or little
loadLight Load
NormalLoad
Heavy Load
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Float &Thermostatic
No ActionUsually
continuous.May cycle.
Usuallycontinuous.May cycle.
Continuous Closed
Inverted BucketSmall
Dribble May dribble Intermittent Continuous Variable
BimetalThermostatic
No ActionUsuallyDribbleAction
May blast athigh
pressuresContinuous Open
ImpulseSmall
Dribble
Usuallycontinuouswith blast athigh loads
Usuallycontinuouswith blast athigh loads
Continuous Open
ThermodynamicDisc
No Action Intermittent Intermittent Continuous Open
Inverted Bucket Steam Trap
The inverted bucket is the most reliable steam trap operating principle known. The heart of its simpledesign is a unique leverage system that multiplies the force provided by the bucket to open the valveagainst pressure. Since the bucket is open at the bottom, it resists damage from water hammers, andwearing points are heavily reinforced for long life.
• intermittent operation - condensate drainage is continuous, discharge is intermittent
• small dribble at no load, intermittent at light and normal load, continuous at full load
• excellent energy conservation
• excellent resistance to wear
• excellent corrosion resistance
• excellent resistance to hydraulic shocks
• vents air and CO2 at steam temperature
• poor ability to vent air at very low pressure
• fair ability to handle start up air loads
• excellent operation against back pressure
• good resistance to damage from freezing
• excellent ability to purge system
• excellent performance on very light loads
• immediate responsiveness to slugs of condensate
•excellent ability to handle dirt
• large comparative physical size
• fair ability to handle flash steam
• open at mechanical failure
Thermostatic Steam Traps
8/8/2019 The Viscosity of a Fluid is Its Resistance to Shear or Flow
http://slidepdf.com/reader/full/the-viscosity-of-a-fluid-is-its-resistance-to-shear-or-flow 28/29
There are two basic designs for the thermostatic steam trap, a bimetallic and a balanced pressuredesign. Both designs use the difference in temperature between live steam and condensate or air tocontrol the release of condensate and air from the steam line.
In an thermostatic bimetallic trap it is common that an oil filled element expands when heated to closea valve against a seat. It may be possible to adjust the discharge temperature of the trap - oftenbetween 60oC and 100oC.
This makes the thermostatic trap suited to get rid of large quantities of air and cold condensate at thestart-up condition. On the other hand the thermostatic trap will have problems to adapt to the variationscommon in modulating heat exchangers.
• intermittent operation
• fair energy conservation
• fair resistance to wear
• good corrosion resistance
• poor resistance to hydraulic shocks (good for bimetal traps)
• do not vent air and CO2 at steam temperature
• good ability to vent air at very low pressure
• excellent ability to handle start up air loads• excellent operation against back pressure
• good resistance to damage from freezing
• good ability to purge system
• excellent performance on very light loads
• delayed responsiveness to slugs of condensate
• fair ability to handle dirt
• small comparative physical size
• poor ability to handle flash steam
• open or closed at mechanical failure depending of the construction
Float Steam Traps
In the float steam trap a valve is connected to a float in such a way that a valve opens when the floatrises.
The float steam trap adapts very well to varying conditions as is the best choice for modulating heatexchangers, but the float steam trap is relatively expensive and not very robust against water hammers.
• continuous operation but may cycle at high pressures
• no action at no load, continuous at full load
• good energy conservation
• good resistance to wear
• good corrosion resistance
• poor resistance to hydraulic shocks
• do not vent air and CO2 at steam temperature
• excellent ability to vent air at very low pressure
• excellent ability to handle start up air loads
• excellent operation against back pressure
• poor resistance to damage from freezing
• fair ability to purge system
• excellent performance on very light loads
• immediate responsiveness to slugs of condensate
8/8/2019 The Viscosity of a Fluid is Its Resistance to Shear or Flow
http://slidepdf.com/reader/full/the-viscosity-of-a-fluid-is-its-resistance-to-shear-or-flow 29/29
• poor ability to handle dirt
• large comparative physical size
• poor ability to handle flash steam
• closed at mechanical failure
Thermodynamic Disc Steam Traps
The thermodynamic trap is an robust steam trap with simple operation. The trap operates by means of the dynamic effect of flash steam as it passes through the trap.
• intermittent operation
• poor energy conservation
• poor resistance to wear
• excellent corrosion resistance
• excellent resistance to hydraulic shocks
• do not vent air and CO2 at steam temperature
• not recommended at low pressure operations
• poor ability to handle start up air loads
• poor operation against back pressure• good resistance to damage from freezing
• excellent ability to purge system
• poor performance on very light loads
• delayed responsiveness to slugs of condensate
• poor ability to handle dirt
• small comparative physical size
• poor ability to handle flash steam
• open at mechanical failure