engineering · heat-transfer-thermal · radiation

Two Surface Thermal Radiation Exchange Calculator

Calculates signed diffuse-gray radiative exchange for an entered two-surface enclosure network or for a small surface in a large isothermal enclosure.

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Calculator overview

Inputs and outputs

This summary comes from the calculator's published input and output contract.

Inputs

RAD Surface 2 Emissivity Conditional
About this input

Total hemispherical gray-body emissivity of surface 2 in enclosure-network mode, from 0 to 1; the active calculation requires a positive value.

Unit fraction Default 0.59 Range 0 to 1
RAD Surface 2 Area m2 Conditional
About this input

Radiating area of surface 2 in enclosure-network mode; it must be at least A1 F12 so that reciprocal F21 does not exceed one.

Unit m^2 Default 3.27 Range At least 0
RAD View Factor 12 Conditional
About this input

Fraction of radiation leaving surface 1 that reaches surface 2. Enter a geometry-derived value; zero does not connect a two-surface enclosure.

Unit fraction Default 0.83 Range 0 to 1
Surface 2 temperature
About this input

Uniform temperature of surface 2 or of the large isothermal enclosure, according to the selected model.

Unit deg C Default 43 Range At least -273.15
RAD Surface 1 Area m2
About this input

Radiating area of surface 1. Zero is a definitional floor but does not form a usable exchange model.

Unit m^2 Default 1.73 Range At least 0
RAD Exchange Mode
About this input

Use the exact two-node enclosure network or the limiting small-surface/large-enclosure relation.

Default Two-surface enclosure network Allowed Two-surface enclosure network, Small surface in large enclosure
RAD Surface 1 Temperature C
About this input

Uniform temperature of surface 1. Values below absolute zero are rejected.

Unit deg C Default 417 Range At least -273.15
RAD Surface 1 Emissivity
About this input

Total hemispherical gray-body emissivity of surface 1, from 0 to 1; the active calculation requires a positive value.

Unit fraction Default 0.71 Range 0 to 1

Outputs

RAD Net Radiation Heat Flux Surface 1 Conditional
About this output

Signed net radiative heat rate divided by surface 1 area.

Unit W/m^2
RAD Implied View Factor 21 Conditional
About this output

View factor from surface 2 to surface 1, obtained from A1 F12 = A2 F21.

Unit fraction
RAD Total Network Resistance Conditional
About this output

Equivalent resistance between blackbody emissive-power nodes; q equals sigma (T1^4 - T2^4) divided by this value.

Unit 1/m^2
RAD Net Radiation Heat Rate Conditional
About this output

Signed net heat rate; positive is from surface 1 to surface 2 or the large enclosure, and negative is toward surface 1.

Unit W
RAD Exchange Direction Conditional
About this output

Direction implied by the two absolute temperatures; equal temperatures give no net exchange.

No unit declared
RAD Blackbody Exchange Fraction Conditional
About this output

Effective gray-body exchange factor divided by the active blackbody geometry factor; structurally bounded from zero to one.

Unit fraction
Model Status
About this output

NOT VALID identifies unusable active temperatures, areas, emissivities, or enclosure geometry; OK means the selected radiation model is internally consistent.

No unit declared
RAD Effective Exchange Factor Conditional
About this output

Combined geometry-emissivity multiplier on A1 sigma (T1^4 - T2^4).

Unit fraction
RAD Blackbody Limit Heat Rate Conditional
About this output

Signed heat rate for black surfaces with the same area, temperatures, and active geometry factor.

Unit W

What it is

The Two-Surface Thermal Radiation Exchange Calculator computes the signed net radiative heat transfer between two opaque, diffuse-gray, isothermal surfaces separated by a medium that neither absorbs nor emits. It runs in two modes: a complete two-surface enclosure network, where you supply both areas, both emissivities and the view factor between them, and the limiting case of a small surface inside a large isothermal enclosure, where only the small surface's own area and emissivity are read.

It reports the net heat rate and the flux referenced to surface 1, the effective gray-body exchange factor, the equivalent network resistance, the reciprocal view factor from surface 2 back to surface 1, the blackbody heat rate for the same geometry, and what fraction of that blackbody limit the gray surfaces reach. The heat rate is signed, so a colder surface 1 correctly reports exchange in the other direction.

It works in SI only: square metres, degrees Celsius internally converted to kelvin, and watts. There is no unit-system selector.

Two things are worth knowing before you start. The calculator supplies no view factor and no emissivity, holds no chart or table for either, and takes both entirely on trust. And an emissivity of exactly zero, though inside the declared range of 0 to 1, is refused by the model rather than treated as a perfect reflector.

It is a screening calculation for surface-to-surface exchange, not a furnace, fire or enclosure design.

Methodology

Purpose and model boundary

This model calculates signed diffuse-gray radiative heat exchange for either a two-surface enclosure network or a small surface inside a large isothermal enclosure. It reports net heat rate, flux, direction, and comparison with the blackbody geometry limit. It does not derive view factors, model participating gases, or include convection, conduction, solar load, or transient behavior.

Inputs and units

Temperatures are entered in degrees Celsius and converted to kelvin before fourth-power calculations. Areas are in square metres, emissivities and view factors are dimensionless, and heat rate is reported in watts. Two-surface mode uses both areas, emissivities, temperatures, and F_12. Large-enclosure mode uses surface 1, the enclosure temperature, and surface-1 emissivity while applying the limiting geometry internally.

Governing relationships

Blackbody emissive power is:

E_b = σ T⁴

For the two-surface enclosure, reciprocity gives:

A_1 F_12 = A_2 F_21

The diffuse-gray network resistances are:

R_surface,1 = (1 - ε_1) / (A_1 ε_1)

R_space = 1 / (A_1 F_12)

R_surface,2 = (1 - ε_2) / (A_2 ε_2)

R_total = R_surface,1 + R_space + R_surface,2

The signed exchange is:

Q = σ (T_1⁴ - T_2⁴) / R_total

In the large-isothermal-enclosure limit:

Q = A_1 ε_1 σ (T_1⁴ - T_2⁴)

The blackbody geometry limit is computed with the same temperatures and geometry but without the gray-surface resistance penalty. Heat flux on surface 1 is q''_1 = Q / A_1.

Calculation sequence

  1. Validate mode, temperatures, active areas, emissivities, and view-factor geometry.
  2. Convert temperatures to absolute kelvin.
  3. In enclosure mode, calculate reciprocal F_21 and both surface plus space resistances; in large-enclosure mode, apply the limiting relationship.
  4. Calculate signed gray-surface heat rate, surface-1 flux, direction, effective exchange factor, and blackbody limit.
  5. Compare gray and blackbody rates and evaluate workbook status.
  6. Generate the temperature-sweep chart from workbook-named series.

Outputs and interpretation

Net radiative heat rate is the headline result. Supporting outputs include heat flux on surface 1, implied reciprocal view factor, total network resistance, exchange direction, effective exchange factor, blackbody limit, and the fraction of that limit achieved by the gray surfaces. A positive result follows the workbook convention of net radiation leaving surface 1.

Validation and status logic

Condition Returned status
Any active temperature, area, emissivity, or view-factor geometry input is invalid NOT VALID: correct active temperatures, areas, emissivities, and view-factor geometry
All active inputs satisfy the workbook model OK

This is the complete named RAD_Model_Status logic. Invalid states return protected zero numeric outputs; they must not be read as a valid no-exchange condition.

Assumptions and limitations

  • Both surfaces are opaque, diffuse-gray, isothermal, and have temperature-independent emissivity.
  • The intervening medium is nonparticipating and does not absorb, emit, or scatter radiation.
  • In two-surface mode, the entered surfaces form the complete enclosure; closure and reciprocity govern the remaining view factors.
  • Large-enclosure mode treats surface 1 as small relative to an isothermal surrounding enclosure.
  • The workbook does not derive F_12; geometry-specific view-factor analysis remains the user's responsibility.
  • Participating gases, spectral/directional effects, semitransparent media, solar irradiation, convection, conduction, and transient temperatures are outside scope.

Restrictions and non-computing states

Active areas, emissivities, and view factors must form a finite supported network. Emissivity is physically bounded from zero to one, but this finite-resistance implementation requires a positive emissivity. Temperatures must be above absolute zero. Values outside the published limits or undeclared options are rejected before the calculation runs.

Errors and warnings

NOT VALID blocks interpretation of every computed output. The workbook has no separate CHECK state; OK confirms only that the declared diffuse-gray model evaluated. Connection, publishing, and calculation-service errors are operational failures, not zero radiation.

References

The resistance network, reciprocity rule, large-enclosure limit, sign convention, named output formulas, and status logic were verified against the delivered workbook, its published input rules, tests, and reviewer packet. The workbook identifies these technical sources:

Frequently asked questions

Why was my zero emissivity rejected if the field allows 0 to 1?
Because the bound and the model are separate gates. The range runs from 0 to 1 and the bound accepts a zero, but the model then returns NOT VALID, because a zero emissivity makes that surface resistance infinite and the network has no finite solution. A perfectly reflective surface is a legitimate idealisation this implementation cannot represent. Enter a small positive value. An emissivity of exactly 1 is accepted and gives a black surface, as is a view factor of 1. A zero view factor is refused: it does not connect the enclosure.
Where do I get the view factor?
Not from here. The calculator holds no view-factor charts and derives nothing from your geometry, so the number you type is taken on trust. It enforces reciprocity, refusing entries whose implied F21 would exceed 1, but it does not test the summation rule and it assumes rather than verifies that your two surfaces form a complete enclosure. Take F12 from a published chart or an integration, and treat this page as arithmetic on a number justified elsewhere.
Which results survive if I get an emissivity wrong?
Three. The blackbody limit, the reciprocal view factor F21 and the exchange direction read only geometry and temperature, so they stay right whatever the emissivities are. On the shipped default, raising surface 1 from 0.71 to 1 lifts the heat rate from 10,740.1 to 13,529.8 watts, up 26 percent, while the limit stays at 17,658.4 and F21 at 0.4391. A view-factor error is worse: raising F12 from 0.83 to 1 moves the heat rate to 11,978.6 and the limit to 21,275.2, leaving no anchor.
Why does the cold surface barely affect the answer?
Because the driving term is a difference of fourth powers. On the shipped default, surface 1 at 690.15 kelvin to the fourth is about 2.27 times ten to the eleventh and surface 2 at 316.15 kelvin about 9.99 times ten to the ninth, roughly four percent of it. For a first estimate you could ignore the cold surface temperature. This is general in radiation, and it is why the hot surface dominates a radiant balance.
What does large-enclosure mode actually change?
It collapses the network to the small surface's own area and emissivity, taking the view factor as 1. The argument is that radiation leaving a small object in a much larger enclosure is absorbed after enough reflections whatever the enclosure is made of. Surface 2's area, its emissivity and the view factor are then hidden and inert: at the shipped temperatures and surface 1, areas of 0 and of a billion square metres both return 15,105.4 watts, as do emissivities of 0 and 1. The F21 output reads 0.
The status says OK on a result that looks absurd. Trust it?
Only as far as the arithmetic. There is no plausibility ceiling here: a surface at 10,000 degrees Celsius covering a million square metres returns OK and about 625 terawatts. OK means the selected model was internally consistent, nothing more. It is not a claim that your geometry exists, that your materials survive those temperatures, or that the diffuse-gray assumption holds there.
Why did every number come back as zero?
Because the model refused the state and zeroed the output block, setting the direction to NOT AVAILABLE. A zero area, a zero emissivity on an active surface, a zero view factor in network mode, an A1 times F12 exceeding A2, and a temperature whose fourth power overflows or whose heat rate underflows to a false zero all do this. Values outside a bound, and blank or null entries, never reach the model. A zero heat rate is not always a refusal: equal temperatures are valid and return zero exchange with status OK. Read the status line first.
Can I use this for a furnace with hot gas?
No. This models exchange between two surfaces separated by a medium that neither absorbs, emits nor scatters. Real furnace gases, carbon dioxide and water vapour in particular, absorb and re-emit strongly in bands, and that participating-medium behaviour often dominates the radiant balance. It is absent here, along with spectral and directional properties, specular reflection, and any surface count above two, as are convection and conduction.
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