Heat Exchanger (G)
Heat exchanger for systems with gas flow and controlled flow.
blockType: EngeeFluids.HeatExchangers.EffectivenessNTU.Gas
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Description
Block Heat Exchanger (G) simulates the heat exchange between the gas flowing between ports A1 and B1 and an external, controlled heat carrier using a scalar signal.
The heat transfer model
The block’s heat transfer model is based on the "efficiency-number of heat transfer units" (E-NTU) method. In steady-state mode, heat exchange is carried out with an efficiency equal to only a fraction of the ideal value, which is achievable in the absence of thermal resistance and constant temperatures at the flow inlet.:
where
-
— actual heat flow;
-
— perfect heat flow;
-
— the fraction of the ideal heat flow actually observed in a real heat exchanger in which there are losses. This value determines the efficiency of the heat exchanger and is a function of the number of transfer units, or .
Dimensionless parameter It reflects the relative efficiency of inter-flow heat exchange in comparison with the ability of streams to accumulate the transferred heat.:
where
-
— coefficient of thermal conductivity between the streams;
-
— the minimum value of the flow heat capacity related to the flow with the least ability to absorb heat.
The flow heat capacity depends on the specific heat capacity of the coolant ( ) and from its mass flow through the heat exchanger ( ):
Efficiency also depends on the relative position of the streams, the number of strokes between them, and the mixing conditions of the streams. Each coolant flow pattern uses its own efficiency expression. The list of such expressions is given in the block E-NTU Heat Transfer.
Flow diagram of heat carriers
Parameter Flow arrangement defines the mutual direction of flows: direct flow, countercurrent, across each other (transverse), as well as the "pipe in a casing" design, in which one flow passes inside the pipes and the other outside, in the casing. The figure below illustrates this flow pattern. The flow in the pipes can make either one stroke through the casing (Fig. on the right) or several strokes (Fig. on the left) for greater heat exchange efficiency.
Alternative flow patterns of heat carriers can be set by general parameterization with tabular efficiency data, which does not require a detailed specification of the heat exchanger. Such data should reflect the flow pattern of the heat carriers, the degree of their mixing, and the number of passages through the casing or pipe.
Mixing conditions
Parameter Cross flow type allows you to set the mixing pattern: one of the streams is mixed, both or none. Mixing involves the transverse movement of the coolant in channels devoid of internal barriers (guides, partitions, ribs or walls). It helps to equalize the temperature gradients in the cross-section. In unmixed streams, as shown in the figure below on the right, the temperature changes only along the flow direction, in mixed streams (Fig. on the left) — both longitudinally and transversely.
The difference between mixed and unmixed flows is taken into account only in the flow patterns of heat carriers with transverse flows, where a longitudinal change in the temperature of one coolant induces transverse temperature gradients in the other. In schemes with direct-flow/countercurrent movement of heat carriers, only longitudinal changes in the temperature of the heat carriers occur and mixing practically does not affect heat transfer, therefore it is not taken into account.
Efficiency curves
Shell-and-tube multi-pass heat exchangers are the most effective (iv.b-e in the figure for 2, 3 and 4 passes). Among single-stroke heat exchangers, countercurrent heat exchangers (ii) are the most efficient, while direct-flow heat exchangers (i) are the least efficient.
Cross-flow heat exchangers occupy an intermediate position in terms of efficiency and their efficiency depends on the degree of mixing. The highest is achieved when there is no mixing in both streams (iii.a), the lowest is achieved when both are mixed (iii.b). Mixing only the stream with the lowest flow heat capacity (iii.c) reduces efficiency to a greater extent than mixing the stream with the highest flow heat capacity (iii.d).
Thermal resistance
Total thermal resistance It represents the sum of local resistances in the direction of heat transfer. These include: convection on the wall surface and thermal conduction through the wall and contaminated layers in the presence of deposits. The formula below is used to calculate the total resistance in the direction from the gas (subscript 1) to the regulated coolant (subscript 2):
where
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and — coefficients of convective heat transfer for gas and controlled coolant;
-
and — the coefficient of deposits on the wall from the side of the gas and the regulated coolant;
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and — the area of the heat transfer surfaces from the gas and the regulated coolant;
-
— thermal resistance of the wall.
The thermal resistance of the wall and the deposition coefficients are constants set in the block parameters. At the same time, heat transfer coefficients are complex functions that depend on the properties of the coolant, flow geometry, and wall friction. They are calculated based on empirical correlations between the Reynolds, Nusselt, and Prandtl numbers. The choice of a specific correlation depends on the flow pattern of the heat carriers and the mixing conditions, and is described in detail in the block E-NTU Heat Transfer, which the block model is based on.
Block structure
A block is a composite component built from simpler blocks. Block Heat Exchanger Interface (G) simulates the gas flow. Scalar signals for the flow heat capacity and heat transfer coefficient, as well as a heat port for temperature, determine the regulated flow. Heat exchange through the wall between the flows is modeled using the block E-NTU Heat Transfer.

Ports
Conserving
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A1
—
gas inlet or outlet
gas
Details
Inlet or outlet port for gas on the corresponding side of the heat exchanger.
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B1
—
gas inlet or outlet
gas
Details
Inlet or outlet port for gas on the corresponding side of the heat exchanger.
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H2
—
inlet temperature of the regulated heat transfer fluid
`heat
Details
Non-directional port related to the inlet temperature of the regulated heat transfer fluid.
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Input
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C2
—
flow heat capacity of the regulated coolant
scalar
Details
Input port that receives the value of the flow heat capacity of the regulated coolant.
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| Complex numbers support |
No |
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HC2
—
heat transfer coefficient of the regulated coolant
scalar
Details
Heat transfer coefficient between the regulated fluid and the separating wall.
| Data types |
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| Complex numbers support |
No |
Parameters
Common
#
Flow arrangement —
flow diagram of heat carriers in the heat exchanger
Parallel or counter flow | Shell and tube | Cross flow | Generic - effectiveness table
Details
The parameter that defines the relative arrangement of the flows in the heat exchanger: direct flow, countercurrent, across each other (transverse), as well as the "pipe in the casing" design, in which one flow passes inside the pipes and the other outside, in the casing.
Alternative flow patterns of heat carriers can be specified in an arbitrary efficiency table, which does not require detailed specifications of the heat exchanger.
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| Evaluatable |
No |
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Wall thermal resistance —
wall resistance to heat flow due to thermal conductivity
K/W
Details
The resistance of the wall to heat flow due to thermal conductivity and the inverse of thermal conductivity, or the product of thermal conductivity by the ratio of surface area to length. The wall resistance is combined with convective resistance and sediment resistance to determine the overall heat transfer coefficient between the flows.
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Yes |
Gas
#
Minimum free-flow area —
the cross-sectional area of the channel at its narrowest point
m^2 | um^2 | mm^2 | cm^2 | km^2 | in^2 | ft^2 | yd^2 | mi^2 | ha | ac
Details
The minimum cross-sectional area of the channel through which the coolant flows between the inlet and outlet. If it is a set of channels, tubes, slits, or grooves, then the value of the parameter is defined as the sum of the smallest areas at the point of the minimum flow area.
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Yes |
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Hydraulic diameter for pressure loss —
the hydraulic diameter of the channel at its narrowest point
m | um | mm | cm | km | in | ft | yd | mi | nmi
Details
The effective internal diameter of the channel in the section with the smallest area. For non—circular channels, the hydraulic diameter is the equivalent diameter of a circle with an area equal to the area of the existing channel. Its value is equal to the ratio of the minimum cross-sectional area of the channel to a quarter of its total perimeter.
If a channel is defined by a set of channels, pipes, slots, or grooves, then the total perimeter is equal to the sum of the perimeters of all the elements. If the channel is a round pipe, then its hydraulic diameter is equal to the actual one.
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Yes |
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Gas volume —
total volume of coolant in the gas channel
m^3 | um^3 | mm^3 | cm^3 | km^3 | ml | l | gal | igal | in^3 | ft^3 | yd^3 | mi^3
Details
The total volume of the coolant contained in the gas channel.
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Yes |
# Laminar flow upper Reynolds number limit — the lower boundary of the transition zone between laminar and turbulent flow regimes
Details
The value of the Reynolds number corresponding to the lower boundary of the transition zone between laminar and turbulent flow regimes. Above this value, inertial forces begin to dominate, as a result of which the flow passes from laminar to turbulent mode. The default value corresponds to a round tube with a smooth inner surface.
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Yes |
# Turbulent flow lower Reynolds number limit — the upper boundary of the transition zone between laminar and turbulent flow regimes
Details
The value of the Reynolds number corresponding to the upper boundary of the transition zone between laminar and turbulent flow regimes. Below this value, viscous forces begin to dominate, as a result of which the flow passes from a turbulent to a laminar regime. The default value corresponds to a round tube with a smooth inner surface.
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Yes |
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Pressure loss model —
mathematical model for calculating pressure losses due to viscous friction
Pressure loss coefficient | Correlation for flow inside tubes | Tabulated data - Darcy friction factor vs. Reynolds number | Tabulated data - Euler number vs. Reynolds number
Details
This parameter allows you to select one of the models for calculating pressure losses due to viscous friction. The parameter determines which expressions will be used in calculating losses, as well as which block parameters must be set at the input. The details of the calculations, depending on the chosen parameterization, are given in the block Heat Exchanger Interface (G).
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No |
# Pressure loss coefficient — total coefficient that takes into account hydraulic losses between ports
Details
The total loss coefficient takes into account all hydraulic flow resistances in the channel, including wall friction losses (major losses) and local resistances due to bends, bends and other geometry changes (minor losses).
The loss coefficient is an empirical dimensionless quantity widely used to describe pressure losses caused by viscous friction. It can be calculated based on experimental data or, in some cases, obtained from technical documentation.
Dependencies
To use this parameter, set for the parameter Pressure loss model meaning Pressure loss coefficient.
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| Evaluatable |
Yes |
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Heat transfer coefficient model —
mathematical model for heat exchange between a heat carrier and a wall
Constant heat transfer coefficient | Correlation for flow inside tubes | Tabulated data - Colburn factor vs. Reynolds number | Tabulated data - Nusselt number vs. Reynolds number and Prandtl number
Details
A mathematical model for heat transfer between a heat carrier and a wall. The choice of the model determines which expressions to use and which parameters to specify for heat transfer calculations.
For more information, see the section E-NTU Heat Transfer.
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| Evaluatable |
No |
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Heat transfer surface area —
the effective surface area used in heat transfer between the heat carrier and the wall
m^2 | um^2 | mm^2 | cm^2 | km^2 | in^2 | ft^2 | yd^2 | mi^2 | ha | ac
Details
The effective surface area used in heat transfer between the heat carrier and the wall. The effective surface area is the sum of the primary and secondary surface areas, the area on which the wall is exposed to the liquid, and the area of the ribs, if any. The surface area of the ribs is usually calculated by the efficiency coefficient of the ribs.
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Yes |
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Gas-wall heat transfer coefficient —
the coefficient of heat transfer during convection between the gas and the wall
W/(m^2*K) | Btu_IT/(hr*ft^2*deltadegR)
Details
The heat transfer coefficient for convection between the gas and the wall. The resistance caused by deposits is taken into account separately in the parameter Fouling factor.
Dependencies
To use this parameter, set for the parameter Heat transfer coefficient model meaning Constant heat transfer coefficient.
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| Evaluatable |
Yes |
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Fouling factor —
thermal resistance due to deposits
K*m^2/W | deltadegR*ft^2*hr/Btu_IT
Details
Thermal resistance due to deposits that form over time on the exposed wall surfaces. Deposits, because they create a new solid layer between the coolant and the wall through which heat must pass, add additional thermal resistance to the heat transfer path. Deposits grow slowly, and the resistance caused by them is assumed to be constant during the simulation.
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| Evaluatable |
Yes |
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Threshold mass flow rate for flow reversal —
threshold mass gas consumption
kg/s | kg/hr | kg/min | g/hr | g/min | g/s | t/hr | lbm/hr | lbm/min | lbm/s
Details
The mass flow rate below which numerical smoothing is applied. This is done in order to avoid interruptions when the flow is stagnant.
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Yes |
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Minimum fluid-wall heat transfer coefficient —
lower bound for the gas heat transfer coefficient
W/(m^2*K) | Btu_IT/(hr*ft^2*deltadegR)
Details
The lower bound for the heat transfer coefficient between the gas and the wall. If the calculation gives a lower heat transfer coefficient, then the value Minimum fluid-wall heat transfer coefficient replaces the calculated value.
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Yes |
Controlled Fluid
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Heat transfer surface area —
the effective surface area used in heat transfer between the heat carrier and the wall
m^2 | um^2 | mm^2 | cm^2 | km^2 | in^2 | ft^2 | yd^2 | mi^2 | ha | ac
Details
The effective surface area used in heat transfer between the heat carrier and the wall. The effective surface area is the sum of the primary and secondary surface areas, the area on which the wall is exposed to the liquid, and the area of the ribs, if any. The surface area of the ribs is usually calculated by the efficiency coefficient of the ribs.
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| Evaluatable |
Yes |
#
Fouling factor —
thermal resistance due to deposits
K*m^2/W | deltadegR*ft^2*hr/Btu_IT
Details
Thermal resistance due to deposits that form over time on the exposed wall surfaces. Deposits, because they create a new solid layer between the coolant and the wall through which heat must pass, add additional thermal resistance to the heat transfer path. Deposits grow slowly, and the resistance caused by them is assumed to be constant during the simulation.
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| Evaluatable |
Yes |
#
Minimum fluid-wall heat transfer coefficient —
the lower limit for the heat transfer coefficient of the regulated coolant
W/(m^2*K) | Btu_IT/(hr*ft^2*deltadegR)
Details
The lower limit for the heat transfer coefficient between the coolant and the wall. If the calculation gives a lower heat transfer coefficient, then the value Minimum fluid-wall heat transfer coefficient replaces the calculated value.
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| Evaluatable |
Yes |
Effects and Initial Conditions
#
Gas initial temperature —
the temperature of the gas in the channel at the beginning of the simulation
K | degC | degF | degR | deltaK | deltadegC | deltadegF | deltadegR
Details
The temperature of the gas in the channel at the beginning of the simulation.
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| Evaluatable |
Yes |
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Gas initial pressure —
the gas pressure in the channel at the beginning of the simulation
Pa | uPa | hPa | kPa | MPa | GPa | kgf/m^2 | kgf/cm^2 | kgf/mm^2 | mbar | bar | kbar | atm | ksi | psi | mmHg | inHg
Details
The gas pressure in the channel at the beginning of the simulation.
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| Evaluatable |
Yes |