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STANDARDS OF THE
TUBULAR EXCHANGER
MANUFACTURERS ASSOCIATION
SECTION 7&8
Prepared by: ATEF Muhammad
Sec. No. 3
Set. No. 110
SECTION 7 (THERMAL RELATIONS)
This section outlines the basic thermal relationships common to most tubular heat transfer equipment.
๏‚ท BASIC HEAT TRANSFER RELATION : ๐ด ๐‘œ =
๐‘„
๐‘ˆโˆ†๐‘ก ๐‘š
๏‚ท OVERALL HEAT TRANSFER COEFFICIENT :
U =
1
[(
1
โ„Ž ๐‘œ
+ ๐‘Ÿ๐‘œ) (
1
โˆˆ๐‘“
) + ๐‘Ÿ๐‘ค + ๐‘Ÿ๐‘– (
๐ด ๐‘œ
๐ด๐‘–
) +
1
โ„Ž๐‘–
(
๐ด ๐‘œ
๐ด๐‘–
)]
๏ƒผ Typical physical factors influencing the determination of fouling
resistances:
o Fluid properties and the propensity for fouling.
o Heat exchanger geometry and orientation.
o Surface and fluid bulk temperatures.
o Local fluid velocities.
o Heat transfer process.
o Fluid treatment.
o Cathodic protection.
๏ƒผ Typical economic factors influencing the determination of appropriate fouling resistances:
o Frequency and amount of cleaning costs.
o Maintenance costs.
o Operating and production costs.
o Longer periods of time on stream.
o Fluid pumping costs.
o Depreciation rates.
o Tax rates.
o Initial cost and variation with size.
o Shut down costs.
o Out-of-service costs.
๏‚ท FLUID TEMPERATURE RELATIONS:
๏ƒผ LOGARITHMIC MEAN TEMPERATURE DIFFERENCE.( For cases of true countercurrent or concurrent
flow)
o to be used must be
o Constant overall heat transfer coefficient
o Complete mixing within any shell cross pass or tube pass
o The number of cross baffles is large โ€™
o Constant flow rate and specific heat
o Enthalpy is a linear function of temperature
The calculation of the overall heat transfer coefficient contains the terms
for the thermal resistances of the fouling layers on the inside and outside
heat transfer surfaces.
These fouling layers are known to increase in thickness with time as the
heat exchanger is operated. Fouling layers normally have a lower thermal
conductivity than the fluids or the tube material,
๐ด ๐‘œ= Required effective outside
heat transfer surface, ft2
๐‘„ = Total heat to be transferred,
BTU/hr.
๐‘ˆ = Overall heat transfer
coefficient, referred to tube
outside surface BTU/hr. ft2 O F
โˆ†๐‘ก ๐‘š= Corrected mean
temperature difference, 0 F
โ„Ž ๐‘œ = Film cbefficient of shell side fluid
โ„Ž๐‘– = Film coefficient of tube side fluid
๐‘Ÿ๐‘œ = Fouling resistance on outside
surface of tubes
๐‘Ÿ๐‘– = Fouling resistance on inside
surface of tubes
๐‘Ÿ๐‘ค = Resistance of tube wall referred
to outside surface of tube wall,
including extended surface if present
FOULING:
Several unique types of fouling mechanisms are currently recognized.
They are individually complex, can occur independently or
simultaneously, and their ratesof development are governed by physical
and chemical relationships dependent on operating conditions. The major
fouling mechanisms are:
Precipitation fouling, particulate fouling, Chemical reaction fouling,
Corrosion fouling and Biological fouling.
o Equal surface in each shell pass or tube pass
o Negligible heat loss to surroundings or internally between passes
๏ƒผ CORRECTION FOR MULTIPASS FLOW
o In multi pass heat exchangers, where there is a combination of concurrent and countercurrent
flow in alternate passes, the mean temperature difference is less than the logarithmic mean
calculated for countercurrent flow and greater than that based on concurrent flow. The correct
mean temperature difference may be evaluated as the product of the logarithmic mean for
countercurrent flow and an LMTD correction factor, F.
๏ƒผ TEMPERATURE EFFECTIVENESS. (defined as the ratio of the temperature change of the tube side
stream to the difference between the two fluid inlet temperatures)
๏‚ท TUBE MEAN METAL TEMPERATURE. (The tube mean metal temperature is dependent on the tube fluid
average temperature and the shell fluid average temperature, the shell and tube heat transfer
coefficients, shell and tube fouling resistances, and tube metal resistance to heat transfer)
๏‚ท Estimation OF SHELL AND TUBE FLUID AVERAGE TEMPERATURES
๏ƒผ ISOTHERMAL SHELL FLUID ISOTHERMAL TUBE FLUID, ALL PASS ARRANGEMENTS.
๏ƒผ ISOTHERMAL SHELL FLUID/LINEAR NONISOTHERMAL TUBE FLUID, ALL PASS ARRANGEMENTS.
๏ƒผ LINEAR NONISOTHERMAL SHELL FLUID/ISOTHERMAL TUBE FLUID, ALL PASS ARRANGEMENTS.
๏ƒผ LINEAR NONISOTHERMAL SHELL AND TUBE FLUIDS, TYPE โ€œEโ€ SHELL.
SECTION 8 (PHYSICAL PROPERTIES OF FLUIDS)
๏ƒผ FLUID DENSITY.
๏ƒผ SPECIFIC GRAVITY OF LIED.
๏ƒผ FRACTIONS and saturated light hydrocarbons.
๏ƒผ DENSITY OF ORGANIC LIQUIDS.
๏ƒผ COMPRESSIBILITY FACTORS FOR GASES AND VAPORS.
๏ƒผ SPECIFIC HEAT.
๏ƒผ LIQUID PETROLEUM FRACTIONS. (functions of temperature)
๏ƒผ PETROLEUMVAPORS. (functions of temperature)
๏ƒผ PURE HYDROCARBON GASES.
๏ƒผ MISCELLANEOUS LIQUIDS AND GASES. (various temperatures)
๏ƒผ GASES AND VAPORS AT ELEVATED PRESSURES.
๏‚ท HEAT CONTENT. (Heat content of petroleum fractions, including the effect of pressure, as functions of
temperature and API gravity for various UOP K values)
๏‚ท THERMAL CONDUCTIVITY.
๏‚ท Viscosity.
These properties is represented in different characteristic graphs

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Tubular Exchanger Standards Sections 7-8

  • 1. STANDARDS OF THE TUBULAR EXCHANGER MANUFACTURERS ASSOCIATION SECTION 7&8 Prepared by: ATEF Muhammad Sec. No. 3 Set. No. 110
  • 2. SECTION 7 (THERMAL RELATIONS) This section outlines the basic thermal relationships common to most tubular heat transfer equipment. ๏‚ท BASIC HEAT TRANSFER RELATION : ๐ด ๐‘œ = ๐‘„ ๐‘ˆโˆ†๐‘ก ๐‘š ๏‚ท OVERALL HEAT TRANSFER COEFFICIENT : U = 1 [( 1 โ„Ž ๐‘œ + ๐‘Ÿ๐‘œ) ( 1 โˆˆ๐‘“ ) + ๐‘Ÿ๐‘ค + ๐‘Ÿ๐‘– ( ๐ด ๐‘œ ๐ด๐‘– ) + 1 โ„Ž๐‘– ( ๐ด ๐‘œ ๐ด๐‘– )] ๏ƒผ Typical physical factors influencing the determination of fouling resistances: o Fluid properties and the propensity for fouling. o Heat exchanger geometry and orientation. o Surface and fluid bulk temperatures. o Local fluid velocities. o Heat transfer process. o Fluid treatment. o Cathodic protection. ๏ƒผ Typical economic factors influencing the determination of appropriate fouling resistances: o Frequency and amount of cleaning costs. o Maintenance costs. o Operating and production costs. o Longer periods of time on stream. o Fluid pumping costs. o Depreciation rates. o Tax rates. o Initial cost and variation with size. o Shut down costs. o Out-of-service costs. ๏‚ท FLUID TEMPERATURE RELATIONS: ๏ƒผ LOGARITHMIC MEAN TEMPERATURE DIFFERENCE.( For cases of true countercurrent or concurrent flow) o to be used must be o Constant overall heat transfer coefficient o Complete mixing within any shell cross pass or tube pass o The number of cross baffles is large โ€™ o Constant flow rate and specific heat o Enthalpy is a linear function of temperature The calculation of the overall heat transfer coefficient contains the terms for the thermal resistances of the fouling layers on the inside and outside heat transfer surfaces. These fouling layers are known to increase in thickness with time as the heat exchanger is operated. Fouling layers normally have a lower thermal conductivity than the fluids or the tube material, ๐ด ๐‘œ= Required effective outside heat transfer surface, ft2 ๐‘„ = Total heat to be transferred, BTU/hr. ๐‘ˆ = Overall heat transfer coefficient, referred to tube outside surface BTU/hr. ft2 O F โˆ†๐‘ก ๐‘š= Corrected mean temperature difference, 0 F โ„Ž ๐‘œ = Film cbefficient of shell side fluid โ„Ž๐‘– = Film coefficient of tube side fluid ๐‘Ÿ๐‘œ = Fouling resistance on outside surface of tubes ๐‘Ÿ๐‘– = Fouling resistance on inside surface of tubes ๐‘Ÿ๐‘ค = Resistance of tube wall referred to outside surface of tube wall, including extended surface if present FOULING: Several unique types of fouling mechanisms are currently recognized. They are individually complex, can occur independently or simultaneously, and their ratesof development are governed by physical and chemical relationships dependent on operating conditions. The major fouling mechanisms are: Precipitation fouling, particulate fouling, Chemical reaction fouling, Corrosion fouling and Biological fouling.
  • 3. o Equal surface in each shell pass or tube pass o Negligible heat loss to surroundings or internally between passes ๏ƒผ CORRECTION FOR MULTIPASS FLOW o In multi pass heat exchangers, where there is a combination of concurrent and countercurrent flow in alternate passes, the mean temperature difference is less than the logarithmic mean calculated for countercurrent flow and greater than that based on concurrent flow. The correct mean temperature difference may be evaluated as the product of the logarithmic mean for countercurrent flow and an LMTD correction factor, F. ๏ƒผ TEMPERATURE EFFECTIVENESS. (defined as the ratio of the temperature change of the tube side stream to the difference between the two fluid inlet temperatures) ๏‚ท TUBE MEAN METAL TEMPERATURE. (The tube mean metal temperature is dependent on the tube fluid average temperature and the shell fluid average temperature, the shell and tube heat transfer coefficients, shell and tube fouling resistances, and tube metal resistance to heat transfer) ๏‚ท Estimation OF SHELL AND TUBE FLUID AVERAGE TEMPERATURES ๏ƒผ ISOTHERMAL SHELL FLUID ISOTHERMAL TUBE FLUID, ALL PASS ARRANGEMENTS. ๏ƒผ ISOTHERMAL SHELL FLUID/LINEAR NONISOTHERMAL TUBE FLUID, ALL PASS ARRANGEMENTS. ๏ƒผ LINEAR NONISOTHERMAL SHELL FLUID/ISOTHERMAL TUBE FLUID, ALL PASS ARRANGEMENTS. ๏ƒผ LINEAR NONISOTHERMAL SHELL AND TUBE FLUIDS, TYPE โ€œEโ€ SHELL. SECTION 8 (PHYSICAL PROPERTIES OF FLUIDS) ๏ƒผ FLUID DENSITY. ๏ƒผ SPECIFIC GRAVITY OF LIED. ๏ƒผ FRACTIONS and saturated light hydrocarbons. ๏ƒผ DENSITY OF ORGANIC LIQUIDS. ๏ƒผ COMPRESSIBILITY FACTORS FOR GASES AND VAPORS. ๏ƒผ SPECIFIC HEAT. ๏ƒผ LIQUID PETROLEUM FRACTIONS. (functions of temperature) ๏ƒผ PETROLEUMVAPORS. (functions of temperature) ๏ƒผ PURE HYDROCARBON GASES. ๏ƒผ MISCELLANEOUS LIQUIDS AND GASES. (various temperatures) ๏ƒผ GASES AND VAPORS AT ELEVATED PRESSURES. ๏‚ท HEAT CONTENT. (Heat content of petroleum fractions, including the effect of pressure, as functions of temperature and API gravity for various UOP K values) ๏‚ท THERMAL CONDUCTIVITY. ๏‚ท Viscosity. These properties is represented in different characteristic graphs