6.3 Solar Heat Gain (SHGC), Fenestration & Cooling Load Temperature Difference / Radiant Time Series (CLTD/RTS)

Key Takeaways

  • Total fenestration heat gain comprises simultaneous thermal conduction and transmitted/absorbed solar radiation: q_fen = U * A * (T_o - T_i) + A * SHGC * IAC * E_t.

  • The Solar Heat Gain Coefficient (SHGC) represents the fraction of incident solar radiation admitted through a window; legacy Shading Coefficient (SC) relates to SHGC by SHGC ≈ 0.86 * SC.

  • Sol-air temperature (T_sol-air) combines outdoor dry-bulb temperature, solar absorptance (alpha), incident solar irradiance (I_t), and surface longwave radiation re-radiation to express the fictitious equivalent outdoor temperature driving envelope conduction.

  • The Cooling Load Temperature Difference (CLTD) method accounts for thermal mass time lag and solar radiation, requiring corrections for indoor temperature setpoint (78°F) and mean outdoor daily temperature (T_o,m = T_peak - DR/2).

  • The Radiant Time Series (RTS) method separates instantaneous heat gains into convective portions (which become immediate cooling load) and radiant portions (which are absorbed by room thermal mass and converted to cooling load over 24 hours via Radiant Time Factors).

Last updated: August 2026

6.3 Solar Heat Gain (SHGC), Fenestration & Cooling Load Temperature Difference / Radiant Time Series (CLTD/RTS)

Solar radiation passing through fenestration and striking opaque exterior envelope surfaces represents one of the largest and most dynamic components of building cooling loads. Unlike steady-state winter heating calculations, cooling load calculations must account for the dual nature of solar radiation: direct optical transmission through glazing, and transient thermal storage within opaque building materials. Engineering methods developed by ASHRAE—including the traditional Cooling Load Temperature Difference (CLTD / SCL / CLF) method and the modern Radiant Time Series (RTS) method—translate instantaneous thermal heat gains into actual cooling loads experienced by the air conditioning system.


1. Fenestration Heat Transfer & Solar Optics

Heat gain through glazed fenestration assemblies (windows, curtain walls, skylights) consists of two concurrent, independent heat transfer mechanisms:

  1. Conductive/Convective Heat Transmission: Driven by the dry-bulb temperature difference across the glass.
  2. Solar Radiation Heat Gain: Driven by direct beam, diffuse sky, and ground-reflected solar irradiance striking the glass surface.
+-----------------------------------------------------------------------------------------+
| FENESTRATION TOTAL HEAT GAIN MECHANISMS                                                 |
+-----------------------------------------------------------------------------------------+
| Incident Solar Irradiance (E_t)                                                         |
|     |                                                                                   |
|     +---> [Reflected Outward] (rho * E_t)                                               |
|     |                                                                                   |
|     +---> [Directly Transmitted] (tau * E_t) -----------------------------> Room Space  |
|     |                                                                            |      |
|     +---> [Absorbed in Glass] (alpha * E_t) --+-> [Inward Re-radiation/Conv] --->+      |
|                                               +-> [Outward Re-radiation/Conv]           |
|                                                                                         |
| Conduction Across Glass:  q_cond = U * A * (T_outdoor - T_indoor)                       |
+-----------------------------------------------------------------------------------------+

Total Fenestration Heat Gain Equation

qfen=qconduction+qsolarq_{\text{fen}} = q_{\text{conduction}} + q_{\text{solar}} qfen=U⋅A⋅(Toutdoor−Tindoor)+A⋅SHGC⋅IAC⋅Etq_{\text{fen}} = U \cdot A \cdot (T_{\text{outdoor}} - T_{\text{indoor}}) + A \cdot \text{SHGC} \cdot \text{IAC} \cdot E_t

Where:

  • qfen=Total instantaneous fenestration heat gain (Btu/hr)q_{\text{fen}} = \text{Total instantaneous fenestration heat gain } (\text{Btu/hr})
  • U=Overall fenestration assembly U-factor, including frame (Btu/(hr⋅ft2⋅∘F))U = \text{Overall fenestration assembly } U\text{-factor, including frame } (\text{Btu/(hr}\cdot\text{ft}^2\cdot{}^\circ\text{F)})
  • A=Total fenestration gross area (ft2)A = \text{Total fenestration gross area } (\text{ft}^2)
  • SHGC=Solar Heat Gain Coefficient of the glazing assembly (dimensionless, 0.0 to 1.0)\text{SHGC} = \text{Solar Heat Gain Coefficient of the glazing assembly (dimensionless, } 0.0\text{ to }1.0)
  • IAC=Interior Attenuation Coefficient (accounting for interior blinds, shades, or drapes)\text{IAC} = \text{Interior Attenuation Coefficient (accounting for interior blinds, shades, or drapes)}
  • Et=Total incident solar irradiance on the surface (Btu/(hr⋅ft2))E_t = \text{Total incident solar irradiance on the surface } (\text{Btu/(hr}\cdot\text{ft}^2))

Solar Heat Gain Coefficient (SHGC) vs. Legacy Shading Coefficient (SC)

  • SHGC: Defined as the fraction of incident solar radiation admitted through a window, both via direct transmission and inward release of absorbed heat: SHGC=τ+Niα\text{SHGC} = \tau + N_i \alpha.
  • Shading Coefficient (SC): Legacy metric defined as the ratio of solar heat gain through a given glazing to that through standard 1/8-inch clear double-strength sheet glass (DSA, SHGCref=0.86\text{SHGC}_{\text{ref}} = 0.86 to 0.870.87).
SHGC=SC×0.86  ⟺  SC=SHGC0.86≈1.163×SHGC\text{SHGC} = \text{SC} \times 0.86 \quad \iff \quad \text{SC} = \frac{\text{SHGC}}{0.86} \approx 1.163 \times \text{SHGC}

Fenestration Shading & Overhang Geometry

External architectural shading devices (horizontal overhangs, vertical fins) block direct solar beam radiation during high sun angles. The Projection Factor (PF) characterizes horizontal overhang depth:

PF=BH\text{PF} = \frac{B}{H}

Where BB is the horizontal overhang projection width (ft) and HH is the vertical distance from the window sill to the bottom of the overhang (ft).


2. Sol-Air Temperature (Tsol-airT_{sol\text{-}air})

Solar radiation striking opaque exterior walls and roofs increases surface temperature significantly above ambient air dry-bulb temperature. The Sol-Air Temperature (Tsol-airT_{sol\text{-}air}) is a fictitious outdoor air temperature that, in the absence of all radiation exchanges, would produce the same total rate of heat transmission into the surface as the combined actual outdoor air temperature, incident solar radiation, and longwave radiant exchange with the sky and surroundings.

Sol-Air Temperature Derivation

Balancing heat flux at the exterior surface:

q/A=ho(To−Ts)+αIt−εΔR=ho(Tsol-air−Ts)q/A = h_o (T_o - T_s) + \alpha I_t - \varepsilon \Delta R = h_o (T_{sol\text{-}air} - T_s) Tsol-air=To+α⋅Itho−ε⋅ΔRhoT_{sol\text{-}air} = T_o + \frac{\alpha \cdot I_t}{h_o} - \frac{\varepsilon \cdot \Delta R}{h_o}

Where:

  • To=Outdoor ambient dry-bulb temperature (∘F)T_o = \text{Outdoor ambient dry-bulb temperature } ({}^\circ\text{F})
  • α=Surface solar absorptance (dimensionless, 0.2 for bright white to 0.95 for black asphalt/tar)\alpha = \text{Surface solar absorptance (dimensionless, } 0.2\text{ for bright white to }0.95\text{ for black asphalt/tar)}
  • It=Total incident solar radiation (direct + diffuse) (Btu/(hr⋅ft2))I_t = \text{Total incident solar radiation (direct + diffuse) } (\text{Btu/(hr}\cdot\text{ft}^2))
  • ho=Exterior surface combined convective and radiative heat transfer coefficient (≈3.0 Btu/(hr⋅ft2⋅∘F))h_o = \text{Exterior surface combined convective and radiative heat transfer coefficient } (\approx 3.0\text{ Btu/(hr}\cdot\text{ft}^2\cdot{}^\circ\text{F)})
  • ε=Surface hemispherical thermal emittance (≈0.90 for most building materials)\varepsilon = \text{Surface hemispherical thermal emittance } (\approx 0.90\text{ for most building materials)}
  • ΔR=Longwave radiation correction factor between surface and sky (Btu/(hr⋅ft2))\Delta R = \text{Longwave radiation correction factor between surface and sky } (\text{Btu/(hr}\cdot\text{ft}^2))
    • Horizontal Roofs: ΔR≈20 Btu/(hr⋅ft2)\Delta R \approx 20\text{ Btu/(hr}\cdot\text{ft}^2) (giving εΔRho≈7∘F\frac{\varepsilon \Delta R}{h_o} \approx 7^\circ\text{F} for horizontal surfaces facing open sky)
    • Vertical Walls: ΔR=0 Btu/(hr⋅ft2)\Delta R = 0\text{ Btu/(hr}\cdot\text{ft}^2) (assuming ground and surroundings are at air temperature, giving εΔRho=0∘F\frac{\varepsilon \Delta R}{h_o} = 0^\circ\text{F})
+-----------------------------------------------------------------------------------------+
| SOL-AIR TEMPERATURE PRACTICAL SHORTCUT FORMULAS (h_o = 3.0 Btu/hr-ft²-°F)              |
+-----------------------------------------------------------------------------------------+
| Horizontal Flat Roofs:     T_sol-air = T_o + (alpha * I_t / 3.0) - 7°F                  |
| Vertical Exterior Walls:   T_sol-air = T_o + (alpha * I_t / 3.0)                        |
+-----------------------------------------------------------------------------------------+

3. Cooling Load Temperature Difference (CLTD) Method

The CLTD / SCL / CLF method is a simplified hand-calculation procedure that accounts for the transient thermal storage and time-delay effects of building envelope assemblies without requiring complex differential equations.

1. Opaque Roofs and Walls Cooling Load

qenvelope=U⋅A⋅CLTDcorrectedq_{\text{envelope}} = U \cdot A \cdot \text{CLTD}_{\text{corrected}}

Where CLTDcorrected\text{CLTD}_{\text{corrected}} modifies tabular baseline CLTD values (which are tabulated for standard conditions: Tindoor=78∘FT_{\text{indoor}} = 78^\circ\text{F}, maximum outdoor temperature To,max=95∘FT_{o,\text{max}} = 95^\circ\text{F}, daily range DR=21∘FDR = 21^\circ\text{F}):

CLTDcorrected=CLTDtable+(78−Tindoor)+(To,m−85)\text{CLTD}_{\text{corrected}} = \text{CLTD}_{\text{table}} + (78 - T_{\text{indoor}}) + (T_{o,m} - 85)

Where the mean outdoor daily temperature To,mT_{o,m} is:

To,m=To,max−DR2T_{o,m} = T_{o,\text{max}} - \frac{DR}{2}

2. Glazing Conduction & Solar Load via CLTD and SCL

qglazing, conduction=U⋅A⋅CLTDcorr, glassq_{\text{glazing, conduction}} = U \cdot A \cdot \text{CLTD}_{\text{corr, glass}} qglazing, solar=A⋅SC⋅SCLq_{\text{glazing, solar}} = A \cdot \text{SC} \cdot \text{SCL}

Where SCL\text{SCL} is the Solar Cooling Load factor (in Btu/(hr⋅ft2)\text{Btu/(hr}\cdot\text{ft}^2)), accounting for solar intensity, latitude, orientation, and room thermal storage mass.

+-----------------------------------------------------------------------------------------+
| THERMAL MASS TIME LAG & DAMPING EFFECT                                                  |
+-----------------------------------------------------------------------------------------+
| Peak Solar Irradiance on Roof occurs at Solar Noon (12:00 PM)                           |
|   - Light Metal Roof (Low Mass):    Peak Cooling Load occurs at 1:00 PM  (1-hr lag)     |
|   - Heavy Concrete Roof (High Mass): Peak Cooling Load occurs at 6:00 PM (6-hr lag)     |
|   *Thermal mass shifts the peak hour and flattens (damps) peak cooling demand!         |
+-----------------------------------------------------------------------------------------+

4. Radiant Time Series (RTS) Method & Periodic Response Factors

The Radiant Time Series (RTS) method is the modern ASHRAE standard for non-residential cooling load calculations. It replaces older transfer function techniques by separating heat gains into convective and radiant components.

1. Convective vs. Radiant Heat Gain Split

All heat gains entering a space are partitioned into two distinct physical fractions:

  • Convective Heat Gain (fcf_c): Heat transferred directly to room air by convection. Becomes instantaneous cooling load immediately.
  • Radiant Heat Gain (fr=1−fcf_r = 1 - f_c): Radiant energy (longwave and shortwave) that passes through air without heating it, striking interior surfaces (floor, partitions, furniture) where it is absorbed and stored.
Heat Gain SourceConvective Fraction (fcf_c)Radiant Fraction (frf_r)Primary Heat Mechanism
Fenestration Solar (without blinds)0.000.001.001.00Shortwave radiation absorbed by floor/furniture
Fenestration Solar (with internal blinds)0.370.370.630.63Blind convection + diffuse radiation
Fenestration Conduction1.001.000.000.00Direct indoor glass surface air convection
Opaque Exterior Walls & Roofs0.000.001.001.00Interior surface radiation exchange
Recessed Fluorescent / LED Lighting0.30 to 0.500.30\text{ to }0.500.50 to 0.700.50\text{ to }0.70Radiation to room surfaces + ceiling plenum air
Occupants (People)0.60 to 0.700.60\text{ to }0.700.30 to 0.400.30\text{ to }0.40Convection from skin/clothing + body radiation
Plug Loads & Computers0.70 to 0.850.70\text{ to }0.850.15 to 0.300.15\text{ to }0.30Internal cooling fan convection + warm casing
Infiltration Air1.001.000.000.00Pure convective air mixing (100% instant)

2. Conduction Time Series Factors (CTSF)

For opaque walls and roofs, the 24-hour conduction heat gain (qe,θq_{e,\theta}) at hour θ\theta is calculated from historical sol-air temperatures using Conduction Time Series Factors (cjc_j):

qe,θ=A∑j=023cj⋅U⋅(Tsol-air,θ−j−Tindoor)q_{e,\theta} = A \sum_{j=0}^{23} c_j \cdot U \cdot \left(T_{sol\text{-}air,\theta - j} - T_{\text{indoor}}\right)

Where ∑j=023cj=1.00\sum_{j=0}^{23} c_j = 1.00. The series factors cjc_j define the precise thermal damping and time delay of the assembly mass.

3. Radiant Time Factors (RTF)

Radiant heat gains (qr,θq_{r,\theta}) generated across the preceding 24 hours are converted into hourly cooling loads (Qr,θQ_{r,\theta}) using zone Radiant Time Factors (rjr_j):

Qr,θ=∑j=023rj⋅qr,θ−jQ_{r,\theta} = \sum_{j=0}^{23} r_j \cdot q_{r,\theta - j}

Where ∑j=023rj=1.00\sum_{j=0}^{23} r_j = 1.00. Total zone sensible cooling load (Qsensible,θQ_{\text{sensible},\theta}) at hour θ\theta is the sum of the instantaneous convective gains and the radiant cooling load:

Qsensible,θ=qconvective,θ+Qr,θQ_{\text{sensible},\theta} = q_{\text{convective},\theta} + Q_{r,\theta}

5. NCEES Reference Handbook Navigation Tactics

  • Fenestration Formulas: Search "Fenestration" or "SHGC" in Section 7 (HVAC & Refrigeration Applications) to find the overall window heat gain equation and typical UU-factors and SHGC\text{SHGC} values for double-pane low-e glass.
  • Sol-Air Temperature: Search "Sol-Air" to access the exact equation Tsol-air=To+(αIt/ho)−(εΔR/ho)T_{sol\text{-}air} = T_o + (\alpha I_t / h_o) - (\varepsilon \Delta R / h_o).
  • CLTD Table Adjustments: Search "CLTD" to find the temperature correction formula CLTDcorr=CLTD+(78−Ti)+(To,m−85)\text{CLTD}_{\text{corr}} = \text{CLTD} + (78 - T_i) + (T_{o,m} - 85).

6. Worked Computational Examples

Example 1: Sol-Air Temperature Calculation for a Flat Commercial Roof

A dark-colored, flat asphalt membrane roof (solar absorptance α=0.90\alpha = 0.90, emittance ε=0.90\varepsilon = 0.90) is exposed to peak solar radiation at solar noon in Phoenix, AZ. The following conditions apply:

  • Outdoor dry-bulb temperature: To=104∘FT_o = 104^\circ\text{F}
  • Total incident solar radiation: It=310 Btu/(hr⋅ft2)I_t = 310\text{ Btu/(hr}\cdot\text{ft}^2)
  • Outside convective heat transfer coefficient: ho=3.0 Btu/(hr⋅ft2⋅∘F)h_o = 3.0\text{ Btu/(hr}\cdot\text{ft}^2\cdot{}^\circ\text{F)}
  • Longwave roof radiation correction factor: ΔR=20 Btu/(hr⋅ft2)\Delta R = 20\text{ Btu/(hr}\cdot\text{ft}^2)

Calculate: (a) The sol-air temperature of the dark roof, and (b) The sol-air temperature if the roof is retrofitted with a bright white "cool roof" elastomeric coating having α=0.25\alpha = 0.25.

Solution:

  1. Sol-air temperature for the dark asphalt roof: Tsol-air=To+α⋅Itho−ε⋅ΔRhoT_{sol\text{-}air} = T_o + \frac{\alpha \cdot I_t}{h_o} - \frac{\varepsilon \cdot \Delta R}{h_o} Tsol-air=104+0.90×3103.0−0.90×203.0T_{sol\text{-}air} = 104 + \frac{0.90 \times 310}{3.0} - \frac{0.90 \times 20}{3.0} Tsol-air=104+93.0−6.0=191.0∘FT_{sol\text{-}air} = 104 + 93.0 - 6.0 = 191.0^\circ\text{F}
  2. Sol-air temperature for the white "cool roof": Tsol-air,cool=104+0.25×3103.0−0.90×203.0T_{sol\text{-}air,\text{cool}} = 104 + \frac{0.25 \times 310}{3.0} - \frac{0.90 \times 20}{3.0} Tsol-air,cool=104+25.83−6.0=123.83∘FT_{sol\text{-}air,\text{cool}} = 104 + 25.83 - 6.0 = 123.83^\circ\text{F}

Conclusion: Retrofitting with a high-albedo cool roof reduces the effective driving temperature difference across the roof by 67.2∘F67.2^\circ\text{F}, drastically reducing roof conductive heat gain.


Example 2: Peak Fenestration Cooling Load Calculation

A west-facing office window assembly has a total area of 250 ft2250\text{ ft}^2. The fenestration consists of double-pane low-e tinted glazing with the following properties:

  • Overall assembly UU-factor: U=0.35 Btu/(hr⋅ft2⋅∘F)U = 0.35\text{ Btu/(hr}\cdot\text{ft}^2\cdot{}^\circ\text{F)}
  • Solar Heat Gain Coefficient: SHGC=0.38\text{SHGC} = 0.38
  • Interior mini-blinds with an Interior Attenuation Coefficient: IAC=0.70\text{IAC} = 0.70
  • Outdoor design dry-bulb: To=96∘FT_o = 96^\circ\text{F}
  • Indoor design setpoint: Ti=74∘FT_i = 74^\circ\text{F}
  • Peak 4:00 PM incident solar irradiance on west facade: Et=215 Btu/(hr⋅ft2)E_t = 215\text{ Btu/(hr}\cdot\text{ft}^2)

Calculate: (a) Fenestration conductive heat gain, (b) Fenestration solar radiation heat gain, and (c) Total instantaneous peak fenestration heat gain.

Solution:

  1. Calculate conductive heat gain: qcond=U⋅A⋅(To−Ti)=0.35×250 ft2×(96−74)∘F=0.35×250×22=1,925 Btu/hrq_{\text{cond}} = U \cdot A \cdot (T_o - T_i) = 0.35 \times 250\text{ ft}^2 \times (96 - 74)^\circ\text{F} = 0.35 \times 250 \times 22 = 1,925\text{ Btu/hr}
  2. Calculate solar radiation heat gain: qsolar=A⋅SHGC⋅IAC⋅Et=250 ft2×0.38×0.70×215 Btu/(hr⋅ft2)q_{\text{solar}} = A \cdot \text{SHGC} \cdot \text{IAC} \cdot E_t = 250\text{ ft}^2 \times 0.38 \times 0.70 \times 215\text{ Btu/(hr}\cdot\text{ft}^2) qsolar=250×0.266×215=14,297.5 Btu/hrq_{\text{solar}} = 250 \times 0.266 \times 215 = 14,297.5\text{ Btu/hr}
  3. Calculate total instantaneous fenestration heat gain: qfen=qcond+qsolar=1,925+14,297.5=16,222.5 Btu/hr=1.352 Tonsq_{\text{fen}} = q_{\text{cond}} + q_{\text{solar}} = 1,925 + 14,297.5 = 16,222.5\text{ Btu/hr} = 1.352\text{ Tons}

(Notice that solar radiation accounts for 88.1% of the total window cooling load!)

Test Your Knowledge

A south-facing window assembly with a total area of 400 ft2 has an overall U-factor of 0.40 Btu/(hr·ft2·°F) and a Solar Heat Gain Coefficient (SHGC) of 0.32. If the indoor space is maintained at 75°F, outdoor temperature is 95°F, incident solar radiation is 180 Btu/(hr·ft2), and no interior shading is present (IAC = 1.0), what is the total instantaneous heat gain through the window?

A

23,040 Btu/hr

B

26,240 Btu/hr

C

3,200 Btu/hr

D

29,440 Btu/hr

Test Your Knowledge

A dark flat roof with solar absorptance alpha = 0.85 and emittance epsilon = 0.90 is exposed to peak noon solar radiation of 300 Btu/(hr·ft2). If the outdoor dry-bulb temperature is 98°F, the outside heat transfer coefficient h_o = 3.0 Btu/(hr·ft2·°F), and the longwave sky radiation correction factor is Delta_R = 20 Btu/(hr·ft2), what is the sol-air temperature of the roof?

A

183.0°F

B

98.0°F

C

177.0°F

D

169.0°F

Test Your Knowledge

An exterior wall has a tabulated baseline CLTD of 18°F at 3:00 PM for standard conditions (78°F indoor setpoint, 95°F maximum outdoor temperature, and 21°F daily range). What is the corrected CLTD if the wall is installed in a building with an indoor setpoint of 74°F, a maximum outdoor design temperature of 100°F, and a daily range of 24°F?

A

21.0°F

B

18.0°F

C

29.0°F

D

25.0°F

Test Your Knowledge

In the ASHRAE Radiant Time Series (RTS) cooling load calculation methodology, how are instantaneous heat gains processed to determine the actual hourly zone sensible cooling load?

A

Convective heat gains become instantaneous cooling loads immediately, while radiant heat gains are absorbed by room surfaces and converted to cooling loads over time using Radiant Time Factors (RTF).

B

All convective and radiant heat gains immediately become instantaneous cooling loads without any time delay.

C

Radiant heat gains become instantaneous cooling loads immediately, while convective gains are delayed by conduction transfer functions.

D

All heat gains are converted to equivalent latent cooling loads using moisture absorption coefficients.

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