heat transfer equations for “thin walled” tubes, a i = a o
TRANSCRIPT
Heat Transfer Equations
For “thin walled” tubes, Ai = Ao
€
˙ Q = UoAΔTm
€
1
Uo
=1
houtside
+x
kw
+1
hinside
FoulingLayers of dirt, particles, biological growth, etc. effect resistance to heat transfer
We cannot predict fouling factors well
Allow for fouling factors when sizing heat transfer equipment
Historical information from similar applications
Little fouling in water side, more on product
ioodirtyo
RRUU
11
,
Log Mean Temperature Difference
For Round, Thin-Walled Tubes
2
1
21
lnT
TTT
Tm
1
2
12
ln2
r
rrr
LAm
Log Mean Temperature Difference
Parallel Flow Counter Flow
Length
Tem
pera
ture
T1 T T2
Length
Tem
pera
ture T1
TT2
Heat LossesTotal Heat Loss = Convection + Radiation
Preventing heat loss, insulation
Air – low thermal conductivity
Air, good
Water – relatively high thermal conductivity
Water, bad
Vessels/pipes above ambient temperature – open pore structure to allow water vapor out
Vessels/pipes below ambient temperature - closed pore structure to avoid condensation
Heat Transfer – Continued
Hot wort at 95C is transferred from one tank to another through a 2.5 cm diameter stainless steel pipe (k = 120 W/m.K, wall thickness 0.1 mm). The pipework is 150 m long and the wort has specific heat capacity of 4.0 kJ/kg.K and density of 975 kg/m3. The heat transfer coefficients on the inside and outside of the pipe are 4000 W/m2K and 125 W/m2K and the temperature of the surroundings is 10C. Assume that the pipe’s wall is “thin.” Approximate the rate of heat loss from the pipe and the exit temperature at the end of the pipe. The velocity in the pipe is 1.0 m/s.
Heat Transfer – ContinuedPrevious Problem continued…
How would adding a 1 cm thick layer of insulation (k = 0.05 W/m.K) to the outer surface of the pipe effect the exit temperature of the wort.
Our pipe has an external emissivity of 0.7. Calculate the heat loss by radiation (without insulation) and compare it to the heat loss by convection.
Refrigeration Terms
• Cooling Load, Cooling Capacity – Qin
• Compressor Load – Win
• Condenser Load – Qout
• Tons of Refrigeration – Rate of Heat Input
• Refrigerant – The Fluid
• Vapor-Compression Refrigeration
• Heat Pump – Same Cycle, Use Qout
Refrigeration
Efficiency = desired output / required input
Desired output = Heat removal from refrigerated space (Qin)
Required input = Work input to compressor
Conservation of Energy: Qin + Win = Qout
COP can be > 1.0
= Cooling Capacity
in
in
W
QCOP
inQ
Refrigeration
• Used when no other method of cooling is available
• Very expensive (40-60% of a brewery’s utility bill)
• Removal of heat from low T source to high T sink
Primary RefrigerantsAmmonia (R-717), R-12, R-134aSaturation temp < Desired application temp
2 to 8C Maturation tanks0 to 1C Beer Chillers-15 to -20C CO2 liquefaction
Typically confined to small region of brewery
Secondary RefrigerantsWater with alcohol or salt solutionsMethanol/glycol, potassium carbonate, NaClLower freezing temperature of waterLow-toxicity (heat exchange with product)Pumped long distances across brewery
Theory and the Cycle
Condenser
Evaporator
Compressor
Qout
Qin
Win
1
23
4
Refrigeration
Applying Conservation of Energy…
12
41
21
32
14
0)(
0)(
0)(
hh
hhCOP
hhmW
hhmQ
hhmQ
in
out
in
Refrigeration1-2: Constant entropy compression (s1 = s2)2-3: Constant pressure heat rejection (3 = sat liq.)3-4: Constant enthalpy throttling4-1: Constant pressure heat addition (1 = sat vap.)
Coefficient of Performance
• Describes how well a refrigeration plant is running
• Heat removed divided by energy input• COP increase with temperature
difference between source and sink
€
COP =Qe
Wc
=h1 − h4
h2 − h1
Typical Manufacturers Performance Curves
Chemical structure of refrigerants
Refrigerant R12, CF2Cl2
Dry Air Fin Condensers• Fluid in condenser does not contact
cooling fluid• High electricity costs for fans
Wet Evaporative Condensers• Fluid in condenser does not contact
cooling fluid• Water sprayed onto tubes to evaporate
and cool
Cooling Tower Condensers• A secondary fluid (water) sprayed• Air passes across water droplets, cools• Forced or induced draft, counter or cross• Cool water to heat exchange condenser
Condenser Selection Considerations• Ambient temperature (Air-fin?)• Ambient humidity (evaporation?)• Space, accessibility, maintenance• Electricity costs (air-fin)• Chemical costs (evaporative, tower)
Legionellosis or L. pneumophila• Major source cooling towers and
evaporative coolers• Name from 1976 meeting of American
Legion – killed 36 people• Kill by heating to 60oC or chlorine
Evaporators and Expansion Devices• Direct expansion with thermostat valve• Regulates flow of liquid being throttled
into evaporator• Diaphragm to balance pressure between
liquid in condenser and sum of evaporator and spring pressure
Evaporators and Expansion Devices• Flooded with level control• Level of liquid in reservoir (typically shell
and tube heat exchanger) controlled with variable throttle valve.
Refrigeration Example
An ideal vapor-compression refrigeration cycle using ammonia operates between the pressures of 2 and 14 bar. The system cools a secondary refrigerant at a rate of 25 kW. Determine:
• The evaporator and condenser temperatures
• The mass flow rate of refrigerant.
• The COP of the system.
• The power consumed by the compressor, in kW