bloc.heat_transfer#
Heat transfer correlations and utilities for reactor modeling.
This module consolidates all heat transfer functions used in Bloc: external natural convection, linearized radiation, thermal resistance networks, gas-to-wall radiative flux, and internal forced convection.
Internal convection delegates to ht.conv_internal which automatically
selects the most accurate applicable correlation for the flow regime.
References
Caleb Bell and Contributors (2016-2025). ht: Heat transfer component of Chemical Engineering Design Library (ChEDL). CalebBell/ht
Attributes#
Functions#
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Thermal resistance for radial conduction in cylindrical geometry. |
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Thermal resistance of a conducto-convective heat transfer surface. |
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Natural convection coefficient at the external wall of a vertical cylinder. |
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Natural convection coefficient at the external wall of a horizontal cylinder. |
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Linearized radiative conductance for small temperature differences. |
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Solve heat transfer through a series thermal resistance stack. |
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Radiative flux from a participating gas to the tube wall in W/m2. |
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Compute internal forced convection coefficient for gas in a circular tube. |
Module Contents#
- bloc.heat_transfer.g = 9.81#
- bloc.heat_transfer.sigma_SB = 5.67e-08#
- bloc.heat_transfer.nu_air_20C = 1.589e-05#
- bloc.heat_transfer.alpha_air_20C = 2.25e-05#
- bloc.heat_transfer.conductivity_air_20C = 0.0263#
- bloc.heat_transfer.Pr_air_20C = 0.707#
- bloc.heat_transfer.thermal_resistance_radial_conduction(diameter, length, conductivity, e_insulation)#
Thermal resistance for radial conduction in cylindrical geometry.
\[R = \frac{\ln(r_2/r_1)}{2\pi k L}, \quad r_1 = D/2, \quad r_2 = D/2 + e_{\mathrm{insulation}}\]- Parameters:
diameter (
float) – Inner diameter in m.length (
float) – Cylinder length in m.conductivity (
float) – Thermal conductivity of insulation in W/m/K.e_insulation (
float) – Insulation thickness in m.
- Returns:
Thermal resistance in K/W.
- Return type:
float
- bloc.heat_transfer.thermal_resistance_CC(h_CC, S)#
Thermal resistance of a conducto-convective heat transfer surface.
\[R = \frac{1}{h_{\mathrm{CC}} \, S}\]- Parameters:
h_CC (
float) – Heat transfer coefficient in W/m2/K.S (
float) – Surface area in m2.
- Returns:
Thermal resistance in K/W.
- Return type:
float
- bloc.heat_transfer.compute_hCC_natConv_vertCyl(diameter, length, T_wall_C, T_amb_C, conductivity=conductivity_air_20C, nu=nu_air_20C, alpha=alpha_air_20C, Pr=Pr_air_20C)#
Natural convection coefficient at the external wall of a vertical cylinder.
Correlation from Taine / Lefevre (1956).
Warning
Valid for laminar flow only; gives low h values.
\[ \begin{align}\begin{aligned}\mathrm{Ra}_L = \frac{g \beta (T_{\mathrm{wall}} - T_{\mathrm{amb}}) L^3}{\nu \alpha}\\\mathrm{Nu} = \frac{4}{3} \left(\frac{7 \mathrm{Ra}_L \mathrm{Pr}}{100 + 105 \mathrm{Pr}}\right)^{1/4} + 0.1143 \frac{272 + 315 \mathrm{Pr}}{64 + 63 \mathrm{Pr}} \frac{L}{D}, \quad h = \frac{\mathrm{Nu} \, k}{L}\end{aligned}\end{align} \]- Parameters:
diameter (
float) – Outer diameter in m.length (
float) – Cylinder length in m.T_wall_C (
float) – Wall temperature in deg C.T_amb_C (
float) – Ambient temperature in deg C.conductivity (
float, optional) – Fluid thermal conductivity in W/m/K. Defaults to air at 20 deg C.nu (
float, optional) – Kinematic viscosity in m2/s. Defaults to air at 20 deg C.alpha (
float, optional) – Thermal diffusivity in m2/s. Defaults to air at 20 deg C.Pr (
float, optional) – Prandtl number. Defaults to air at 20 deg C.
- Returns:
Convective heat transfer coefficient h in W/m2/K.
- Return type:
float
- bloc.heat_transfer.compute_hCC_natConv_horizCyl(diameter, length, T_wall_C, T_amb_C, conductivity=conductivity_air_20C, nu=nu_air_20C, alpha=alpha_air_20C, Pr=Pr_air_20C)#
Natural convection coefficient at the external wall of a horizontal cylinder.
Uses Churchill & Chu (1975) correlation.
\[ \begin{align}\begin{aligned}\mathrm{Ra}_D = \frac{g \beta (T_{\mathrm{wall}} - T_{\mathrm{amb}}) D^3}{\nu \alpha}\\\mathrm{Nu}_D = \left(0.6 + \frac{0.387 \mathrm{Ra}_D^{1/6}} {(1 + (0.559/\mathrm{Pr})^{9/16})^{8/27}}\right)^2, \quad h = \frac{\mathrm{Nu}_D \, k}{D}\end{aligned}\end{align} \]- Parameters:
diameter (
float) – Outer diameter in m.length (
float) – Cylinder length in m (unused in this correlation, kept for API consistency).T_wall_C (
float) – Wall temperature in deg C.T_amb_C (
float) – Ambient temperature in deg C.conductivity (
float, optional) – Fluid thermal conductivity in W/m/K. Defaults to air at 20 deg C.nu (
float, optional) – Kinematic viscosity in m2/s. Defaults to air at 20 deg C.alpha (
float, optional) – Thermal diffusivity in m2/s. Defaults to air at 20 deg C.Pr (
float, optional) – Prandtl number. Defaults to air at 20 deg C.
- Returns:
Convective heat transfer coefficient h in W/m2/K.
- Return type:
float
- bloc.heat_transfer.compute_hrad_linearRadiation(eps, Tmoy)#
Linearized radiative conductance for small temperature differences.
\[h_{\mathrm{rad}} = \varepsilon \sigma_{\mathrm{SB}} \, 4 T_{\mathrm{moy}}^3\]- Parameters:
eps (
float) – Emissivity, dimensionless.Tmoy (
float) – Mean temperature in K.
- Returns:
Linearized radiative heat transfer coefficient in W/m2/K.
- Return type:
float
- bloc.heat_transfer.compute_heat_losses_linear(Tr_C, Tamb_C, R_list)#
Solve heat transfer through a series thermal resistance stack.
\[R_{\mathrm{tot}} = \sum_i R_i, \quad \Phi = \frac{T_{\mathrm{reac}} - T_{\mathrm{amb}}}{R_{\mathrm{tot}}}, \quad \Delta T_i = \Phi \, R_i\]- Parameters:
Tr_C (
float) – Temperature inside the reactor in deg C.Tamb_C (
float) – Ambient temperature in deg C.R_list (
listoffloat) – Thermal resistances in K/W, ordered from reactor interior to ambient.
- Returns:
{"Phi": float, "T_reac": float, "T_wall_ext": float, "T_amb": float, ...}wherePhiis heat loss in W.- Return type:
dict
- bloc.heat_transfer.compute_gas2wall_radiative_flux(T_g, T_w, kappa_grey, D)#
Radiative flux from a participating gas to the tube wall in W/m2.
Uses the grey gas approximation with cylindrical geometry (mean beam length approximation via spherical integral).
Assumptions:
Temperature and composition are uniform in the cross-section.
Grey body gas with absorption coefficient
kappa_grey.Walls are black (covered by soot); no wall reflection.
\[ \begin{align}\begin{aligned}f_{\mathrm{trans}} = 2 \int_0^{\pi/2} e^{-\kappa D \cos\theta} \cos^2\theta \sin\theta \, d\theta\\q_{\mathrm{rad}} = \left(\frac{2}{3} - f_{\mathrm{trans}}\right) \sigma_{\mathrm{SB}} (T_g^4 - T_w^4)\end{aligned}\end{align} \]Positive
q_radmeans net heat transfer from gas to wall.- Parameters:
T_g (
float) – Gas temperature in K.T_w (
float) – Wall temperature in K.kappa_grey (
float) – Grey gas absorption coefficient in 1/m. Usekappa_grey = 0to disable gas radiation.D (
float) – Tube inner diameter in m.
- Returns:
q_rad (
float) – Net radiative heat flux from gas to wall in W/m2.f_trans (
float) – Transmittance factor (dimensionless).
- bloc.heat_transfer.internal_convection_h(diameter, mass_flow_rate, gas, x_position=None)#
Compute internal forced convection coefficient for gas in a circular tube.
Delegates to
ht.conv_internal.Nu_conv_internal()[CalebBell_ht] which dynamically selects the most accurate applicable correlation:Laminar developing flow (Re < 2300,
x_positionprovided): Baehr-Stephan laminar thermal/velocity entry.Laminar fully-developed (Re < 2300, no
x_position): Constant wall temperature, Nu = 3.66.Turbulent with entry effects (Re > 4000,
x_positionprovided): Hausen.Turbulent general (Re > 4000): Churchill-Zajic.
Turbulent, low Prandtl (Pr < 0.03): Martinelli.
Transport properties (viscosity, thermal conductivity, heat capacity) are read from the Cantera
Solutionobject at the current state. The gas mechanism must define a transport model (e.g. Mix or Multi); mechanisms withtransport_model == 'none'are not supported.- Parameters:
diameter (
float) – Tube inner diameter in m.mass_flow_rate (
float) – Mass flow rate through the tube in kg/s.gas (
cantera.Solution) – Gas object at the current thermodynamic state (must have transport).x_position (
floatorNone, optional) – Distance from the tube inlet in m. When provided, entry-length correlations are used; otherwise fully-developed flow is assumed.
- Returns:
Convective heat transfer coefficient h in W/m2/K.
- Return type:
float- Raises:
ValueError – If
gas.transport_model == 'none'(mechanism has no transport data).
See also
ht.conv_internal.Nu_conv_internalUnderlying correlation selector from the ht library.
Notes
For CH4 pyrolysis conditions (10 SLM, D = 100 mm), Re ~ 130–250 across the full temperature range (25–1600 deg C), so fully-developed laminar flow applies and Nu = 3.66. Radiation dominates at high temperatures.