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Heat Exchanger Networking
How we will study networking
• Basics of energy balance
• Basics of energy recovery
• Pinch concept
Unsteady state Energy Balance
• In a batch process
• In processes where rate of energy generation
or removal is unsteady
• Differential energy balance is to be set up
Differential energy balance
• we will solve numerical
Energy Recovery
• From Process streams at high pressure or temperature,
• Or which contain combustible material containing energy
that can be usefully recovered.
• Factors which will determine energy recovery would be:
 The value of the energy that can be usefully extracted
 The cost of recovery
 The value of the energy will depend on the primary cost of
energy at the site.
• It may be worth while recovering energy from a
process stream at a site where energy costs are
high but not where the primary energy costs are
low.
• The cost of recovery will be the capital and
operating cost of any additional equipment
required.
• If the savings exceed the operating cost, including
capital charges, then the energy recovery will
usually be worthwhile.
• Maintenance costs should be included in the
operating cost
Heat Exchange
• The most common energy-recovery technique is to
utilise the heat in a high-temperature process stream
to heat a colder stream
• It will save steam costs; and also cooling water, if the
hot stream requires cooling.
• Conventional shell and tube exchangers are normally
used.
More total heat-transfer area will be needed, over
that for steam heating and water cooling, as the
overall driving forces will be smaller.
• The cost of recovery will be reduced if the streams are
located conveniently close.
The amount of energy that can be recovered will depend on the
• Temperature
• Flow,
• Heat capacity,
• and temperature change possible, in each stream.
• A reasonable temperature driving force must be maintained to
keep the exchanger area to a practical size.
• The most efficient exchanger will be the one in which the shell and
tube flows are truly countercurrent.
• Multiple tube pass exchangers are usually used for practical
reasons.
• With multiple tube passes the flow will be part counter-current and
part co-current and temperature crosses can occur, which will
reduce the efficiency of heat recovery
• The hot process streams leaving a reactor or a
distillation column are frequently used to
preheat the feedstreams
Heat Exchanger Netwroks
• In an industrial process there will be many hot
and cold streams and
Chemical Engineers search for
An optimum arrangement of the streams for
energy recovery by heat exchange
Consider that there are M hot streams, 1, 2,
3, . . .,M to be cooled and N cold streams 1,
2, 3, . . . ,N to be heated;
Each stream having some inlet temperature
or an outlet temperature and a stream heat
capacity .
There may also be L 1, 2, 3, . . . ,L auxiliary
steam heated or water-cooled exchangers.
• Search :
• To create a minimum cost network of
exchangers, that will also meet the design
specifications on the required outlet
temperature of each stream.
• Computer Time for searching an optimum low
cost network of exchangers will be very large
if only mathematical approach is followed
Waste Heat Boilers
• If the process streams are at a sufficiently high
temperature the heat recovered can be used to gener ate
steam.
• Waste-heat boilers are often used to recover heat from
furnace flue gases and the process gas streams from high-
temperature reactors.
• The pressure, and superheat temperature, of the stream
generated will depend on the temperature of the hot
stream and the approach temperature permissible at the
boiler exit .
• As with any heat-transfer equipment, the area required
will increase as the mean temperature driving force (log
mean T) is reduced.
• The permissible exit temperature may also be
limited by process considerations.
• If the gas stream contains water vapour and
soluble corrosive gases, such as HCl or SO2,
the exit gases temperature must be kept
above the dew point.
Reformed gas waste-heat boiler arrangement of
vertical U-tube water-tube boiler
High Temperature Reactors
• If a reaction is highly exothermic, cooling will
be needed and, if the reactor temperature is
high enough, the heat removed can be used
to generate steam.
• The lowest steam pressure normally used in
the process industries is 2.7 bar (25 psig) and
steam is normally distributed at a header
pressure of around 8 bar (100 psig); so any
reactor with a temperature above 200C is a
potential steam generator
Low Cost Alternative Fuels
• The waste products from any process (gases,
liquids and solids) which contain significant
quantities of combustible material can be
used as low-grade fuels; for raising steam or
direct process heating.
• The off-gases (vent gas) from reactors, and
recycle stream purges are often of high
enough calorific value to be used as fuel
• Other factors which, together with the
calorific value, will determine the economic
value of an off-gas as a fuel are the quantity
available and the continuity of supply.
• Waste gases are best used for steam raising,
rather than for direct process heating, as this
decouples the source from the use and gives
greater flexibility.
Combustible Solid and Liquid Wastes
• Combustible liquid and solid waste can be
disposed of by burning, which is usually
preferred to dumping
Heat Pump
• A heat pump is a device for raising low grade
heat to a temperature at which the heat can
be utilised.
• It pumps the heat from a low temperature
source to the higher temperature sink, using a
small amount of energy relative to the heat
energy recovered.
• Heat pumps are increasingly finding
applications in the process industries.
• A typical application is the use of the low
grade heat from the condenser of a
distillation column to provide heat for
the reboiler.
• Heat pumps are also used with dryers,
heat being abstracted from the exhaust
air and used to preheat the incoming air.
• The “efficiency” of a heat pump is measured by the
coefficient of performance, COP:
Process Integration and Pinch
Technology
• Process integration can lead to a substantial
reduction in the energy requirements of a
process.
• Pinch Technology is used for investigating
energy integration and the efficient design of
heat exchanger networks;
• The term derives from the fact that in a plot of
the system temperatures versus the heat
transferred, a pinch usually occurs between
the hot stream and cold stream curves.
(shown in next figure)
• The pinch represents a distinct
thermodynamic break in the system and that,
for minimum energy requirements, heat
should not be transferred across the pinch
Pinch Technology
Simple Two Stream Problem
• The heat transferred between the streams is shown
on the diagram as delta Hex, and the heat
transferred from the streams as ΔHcoldand ΔHhot:
• ΔHhot= Cp * temperature change
• The amount of heating and cooling needed will
depend on the minimum temperature difference.
• Decreasing ΔTmin will increase the amount of heat
exchanged between the two streams and so
decrease the consumption of the hot and cold
utilities.
Four Stream Problem
• As for the two-stream problem, the displacement of
the curves at the top and bottom of the diagram
gives the hot and cold utility requirements.
• These will be the minimum values needed to satisfy
the target temperatures.
• It gives the designer target values for the utilities to
aim for when designing the exchanger network.
• Any design can be compared with the minimum
utility requirements to check if further improvement
is possible.
• In most exchanger networks the minimum
temperature difference will occur at only
one point. This is termed the pinch.
• In the problem being considered, the pinch
occurs at between 90C on the hot stream
curve and 80C on the cold stream curve.
Significance of the Pinch
• The pinch divides the system into two distinct
thermodynamic regions.
• The region above the pinch can be considered
a heat sink, with heat flowing into it, from the
hot utility, but not out of it.
• Below the pinch the converse is true.
• Heat flows out of the region to the cold utility.
• No heat flows across the pinch.
• If a network is designed that requires heat to
flow across the pinch, then the consumption
of the hot and cold utilities will be greater
than the minimum values that could be
achieved.
The Problem Table Method
5. “Cascade” the heat surplus from one interval to the next down the
column of interval temperatures; Figure 3.23a.
• 6. Introduce just enough heat to the top of the
cascade to eliminate all the negative values;
see Figure 3.23b.
• Summary
• For maximum heat recovery and minimum
use of utilities:
• 1. Do not transfer heat across the pinch
• 2. Do not use hot utilities below the pinch
• 3. Do not use cold utilities above the pinch
Grid Representation
• The stream heat capacities CP are shown in a
column at the end of the stream lines.
Network design for maximum energy recovery
• Previous analysis carried has shown
that the minimum utility
requirements for the problem set
out are 50 kW of the hot and 30 kW
of the cold utility
• Also that the pinch occurs where the
cold streams are at 80 and the hot
90C.
The vertical dotted lines
represent the pinch and separate the grid into the
regions above and below the pinch.
• For maximum energy recovery (minimum
utility consumption) the best performance is
obtained if no cooling is used above the pinch.
This means that the hot streams above the
pinch should be brought to the pinch
temperature solely by exchange with the cold
streams.
Network Design Above The Pinch
• CPhot ≤ Cpcold
1. Applying this condition at the pinch, stream 1 can be
matched with stream 4, but not with 3.
• Matching streams 1 and 4 and transferring the full
amount of heat required to bring stream 1 to the
pinch temperature gives:
Network Design Below The Pinch
Minimum No of Exchangers
• In Figure 3.27 it is clear that there is scope for
reducing the number of exchangers.
• Exchanger D can be deleted and the heat
loads of the cooler and heater increased to
bring streams 2 and 3 to their target
temperatures.
• Heat would cross the pinch and the
consumption of the utilities would be
increased.
• Whether the revised network would be
better, more economic, would depend on the
relative cost of capital and utilities.
• For any network there will be an optimum
design that gives the least annual cost: capital
charges plus utility and other operating costs.
• To find the optimum design it will be
necessary to cost a number of alternative
designs, seeking a compromise between the
capital costs, determined by the number and
size of the exchangers, and the utility costs,
determined by the heat recovery achieved.
• For simple networks Holmann (1971) has shown
that the minimum number of exchangers is given
by:
Summary For Optimum design of Network
1. Start with the design for maximum heat
recovery. The number of exchangers needed
will be equal to or less than the number for
maximum energy recovery.
2. Identify loops that cross the pinch. The design
for maximum heat recovery will usually
contain loops.
3. Starting with the loop with the least heat
load, break the loops by adding or subtracting
heat.
4. Check that the specified minimum
temperature difference ΔTmin has not been
violated, and revise the design as necessary to
restore the ΔTmin.
5. Estimate the capital and operating costs, and
the total annual cost.
6. Repeat the loop breaking and network
revision to find the lowest cost design.
7. Consider the safety, operability and
maintenance aspects of the proposed design.
Importance of Minimum Temperature Difference
• The value chosen for Tmin will determine the size of the
heat exchangers in a network.
• Reducing Tmin will increase the heat recovery, decreasing
the utility consumption and cost, but at the expense of an
increase in the exchanger size and capital cost.
• For any network there will be a best value for the minimum
temperature difference that will give the lowest total annual
costs.
• The effect of changes in the specified Tmin need to be
investigated when optimising a heat recovery system.
Heat exchanger networking

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Heat exchanger networking

  • 2. How we will study networking • Basics of energy balance • Basics of energy recovery • Pinch concept
  • 3. Unsteady state Energy Balance • In a batch process • In processes where rate of energy generation or removal is unsteady • Differential energy balance is to be set up
  • 4. Differential energy balance • we will solve numerical
  • 5. Energy Recovery • From Process streams at high pressure or temperature, • Or which contain combustible material containing energy that can be usefully recovered. • Factors which will determine energy recovery would be:  The value of the energy that can be usefully extracted  The cost of recovery  The value of the energy will depend on the primary cost of energy at the site.
  • 6. • It may be worth while recovering energy from a process stream at a site where energy costs are high but not where the primary energy costs are low. • The cost of recovery will be the capital and operating cost of any additional equipment required. • If the savings exceed the operating cost, including capital charges, then the energy recovery will usually be worthwhile. • Maintenance costs should be included in the operating cost
  • 7. Heat Exchange • The most common energy-recovery technique is to utilise the heat in a high-temperature process stream to heat a colder stream • It will save steam costs; and also cooling water, if the hot stream requires cooling. • Conventional shell and tube exchangers are normally used. More total heat-transfer area will be needed, over that for steam heating and water cooling, as the overall driving forces will be smaller. • The cost of recovery will be reduced if the streams are located conveniently close.
  • 8. The amount of energy that can be recovered will depend on the • Temperature • Flow, • Heat capacity, • and temperature change possible, in each stream. • A reasonable temperature driving force must be maintained to keep the exchanger area to a practical size. • The most efficient exchanger will be the one in which the shell and tube flows are truly countercurrent. • Multiple tube pass exchangers are usually used for practical reasons. • With multiple tube passes the flow will be part counter-current and part co-current and temperature crosses can occur, which will reduce the efficiency of heat recovery
  • 9. • The hot process streams leaving a reactor or a distillation column are frequently used to preheat the feedstreams
  • 10. Heat Exchanger Netwroks • In an industrial process there will be many hot and cold streams and Chemical Engineers search for An optimum arrangement of the streams for energy recovery by heat exchange
  • 11.
  • 12. Consider that there are M hot streams, 1, 2, 3, . . .,M to be cooled and N cold streams 1, 2, 3, . . . ,N to be heated; Each stream having some inlet temperature or an outlet temperature and a stream heat capacity . There may also be L 1, 2, 3, . . . ,L auxiliary steam heated or water-cooled exchangers.
  • 13. • Search : • To create a minimum cost network of exchangers, that will also meet the design specifications on the required outlet temperature of each stream. • Computer Time for searching an optimum low cost network of exchangers will be very large if only mathematical approach is followed
  • 14. Waste Heat Boilers • If the process streams are at a sufficiently high temperature the heat recovered can be used to gener ate steam. • Waste-heat boilers are often used to recover heat from furnace flue gases and the process gas streams from high- temperature reactors. • The pressure, and superheat temperature, of the stream generated will depend on the temperature of the hot stream and the approach temperature permissible at the boiler exit . • As with any heat-transfer equipment, the area required will increase as the mean temperature driving force (log mean T) is reduced.
  • 15. • The permissible exit temperature may also be limited by process considerations. • If the gas stream contains water vapour and soluble corrosive gases, such as HCl or SO2, the exit gases temperature must be kept above the dew point.
  • 16. Reformed gas waste-heat boiler arrangement of vertical U-tube water-tube boiler
  • 17. High Temperature Reactors • If a reaction is highly exothermic, cooling will be needed and, if the reactor temperature is high enough, the heat removed can be used to generate steam. • The lowest steam pressure normally used in the process industries is 2.7 bar (25 psig) and steam is normally distributed at a header pressure of around 8 bar (100 psig); so any reactor with a temperature above 200C is a potential steam generator
  • 18.
  • 19. Low Cost Alternative Fuels • The waste products from any process (gases, liquids and solids) which contain significant quantities of combustible material can be used as low-grade fuels; for raising steam or direct process heating. • The off-gases (vent gas) from reactors, and recycle stream purges are often of high enough calorific value to be used as fuel
  • 20. • Other factors which, together with the calorific value, will determine the economic value of an off-gas as a fuel are the quantity available and the continuity of supply. • Waste gases are best used for steam raising, rather than for direct process heating, as this decouples the source from the use and gives greater flexibility.
  • 21. Combustible Solid and Liquid Wastes • Combustible liquid and solid waste can be disposed of by burning, which is usually preferred to dumping
  • 22.
  • 23. Heat Pump • A heat pump is a device for raising low grade heat to a temperature at which the heat can be utilised. • It pumps the heat from a low temperature source to the higher temperature sink, using a small amount of energy relative to the heat energy recovered.
  • 24. • Heat pumps are increasingly finding applications in the process industries. • A typical application is the use of the low grade heat from the condenser of a distillation column to provide heat for the reboiler. • Heat pumps are also used with dryers, heat being abstracted from the exhaust air and used to preheat the incoming air.
  • 25.
  • 26. • The “efficiency” of a heat pump is measured by the coefficient of performance, COP:
  • 27. Process Integration and Pinch Technology • Process integration can lead to a substantial reduction in the energy requirements of a process. • Pinch Technology is used for investigating energy integration and the efficient design of heat exchanger networks;
  • 28. • The term derives from the fact that in a plot of the system temperatures versus the heat transferred, a pinch usually occurs between the hot stream and cold stream curves. (shown in next figure) • The pinch represents a distinct thermodynamic break in the system and that, for minimum energy requirements, heat should not be transferred across the pinch
  • 29.
  • 31.
  • 32. Simple Two Stream Problem
  • 33.
  • 34. • The heat transferred between the streams is shown on the diagram as delta Hex, and the heat transferred from the streams as ΔHcoldand ΔHhot: • ΔHhot= Cp * temperature change • The amount of heating and cooling needed will depend on the minimum temperature difference. • Decreasing ΔTmin will increase the amount of heat exchanged between the two streams and so decrease the consumption of the hot and cold utilities.
  • 36.
  • 37. • As for the two-stream problem, the displacement of the curves at the top and bottom of the diagram gives the hot and cold utility requirements. • These will be the minimum values needed to satisfy the target temperatures. • It gives the designer target values for the utilities to aim for when designing the exchanger network. • Any design can be compared with the minimum utility requirements to check if further improvement is possible.
  • 38. • In most exchanger networks the minimum temperature difference will occur at only one point. This is termed the pinch. • In the problem being considered, the pinch occurs at between 90C on the hot stream curve and 80C on the cold stream curve.
  • 39. Significance of the Pinch • The pinch divides the system into two distinct thermodynamic regions. • The region above the pinch can be considered a heat sink, with heat flowing into it, from the hot utility, but not out of it. • Below the pinch the converse is true. • Heat flows out of the region to the cold utility.
  • 40. • No heat flows across the pinch. • If a network is designed that requires heat to flow across the pinch, then the consumption of the hot and cold utilities will be greater than the minimum values that could be achieved.
  • 42.
  • 43.
  • 44.
  • 45.
  • 46. 5. “Cascade” the heat surplus from one interval to the next down the column of interval temperatures; Figure 3.23a.
  • 47.
  • 48. • 6. Introduce just enough heat to the top of the cascade to eliminate all the negative values; see Figure 3.23b.
  • 49. • Summary • For maximum heat recovery and minimum use of utilities: • 1. Do not transfer heat across the pinch • 2. Do not use hot utilities below the pinch • 3. Do not use cold utilities above the pinch
  • 51. • The stream heat capacities CP are shown in a column at the end of the stream lines.
  • 52.
  • 53. Network design for maximum energy recovery • Previous analysis carried has shown that the minimum utility requirements for the problem set out are 50 kW of the hot and 30 kW of the cold utility • Also that the pinch occurs where the cold streams are at 80 and the hot 90C.
  • 54. The vertical dotted lines represent the pinch and separate the grid into the regions above and below the pinch.
  • 55. • For maximum energy recovery (minimum utility consumption) the best performance is obtained if no cooling is used above the pinch. This means that the hot streams above the pinch should be brought to the pinch temperature solely by exchange with the cold streams.
  • 56.
  • 57. Network Design Above The Pinch • CPhot ≤ Cpcold 1. Applying this condition at the pinch, stream 1 can be matched with stream 4, but not with 3. • Matching streams 1 and 4 and transferring the full amount of heat required to bring stream 1 to the pinch temperature gives:
  • 58.
  • 59.
  • 60.
  • 61. Network Design Below The Pinch
  • 62.
  • 63.
  • 64.
  • 65.
  • 66. Minimum No of Exchangers
  • 67. • In Figure 3.27 it is clear that there is scope for reducing the number of exchangers. • Exchanger D can be deleted and the heat loads of the cooler and heater increased to bring streams 2 and 3 to their target temperatures.
  • 68. • Heat would cross the pinch and the consumption of the utilities would be increased. • Whether the revised network would be better, more economic, would depend on the relative cost of capital and utilities. • For any network there will be an optimum design that gives the least annual cost: capital charges plus utility and other operating costs.
  • 69. • To find the optimum design it will be necessary to cost a number of alternative designs, seeking a compromise between the capital costs, determined by the number and size of the exchangers, and the utility costs, determined by the heat recovery achieved.
  • 70. • For simple networks Holmann (1971) has shown that the minimum number of exchangers is given by:
  • 71.
  • 72.
  • 73. Summary For Optimum design of Network 1. Start with the design for maximum heat recovery. The number of exchangers needed will be equal to or less than the number for maximum energy recovery. 2. Identify loops that cross the pinch. The design for maximum heat recovery will usually contain loops. 3. Starting with the loop with the least heat load, break the loops by adding or subtracting heat.
  • 74. 4. Check that the specified minimum temperature difference ΔTmin has not been violated, and revise the design as necessary to restore the ΔTmin. 5. Estimate the capital and operating costs, and the total annual cost. 6. Repeat the loop breaking and network revision to find the lowest cost design. 7. Consider the safety, operability and maintenance aspects of the proposed design.
  • 75. Importance of Minimum Temperature Difference • The value chosen for Tmin will determine the size of the heat exchangers in a network. • Reducing Tmin will increase the heat recovery, decreasing the utility consumption and cost, but at the expense of an increase in the exchanger size and capital cost. • For any network there will be a best value for the minimum temperature difference that will give the lowest total annual costs. • The effect of changes in the specified Tmin need to be investigated when optimising a heat recovery system.