Building Science & Enclosure PhysicsASHRAE Fundamentals Ch. 1 & 26Glaser Method (EN ISO 13788)IRC Sec. R702.7

Psychrometrics & Building Envelope Physics: Condensation Dynamics & Hydrothermal Gradients

A technical reference detailing how moist air thermodynamics, vapor pressure gradients, and multi-layer wall assembly thermal transmission interact in steady-state models of interstitial condensation and moisture control.

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1. The Thermodynamic Basis: Moist Air & Building Enclosures

Building envelope analysis applies moist air psychrometrics to multi-layered assemblies. While HVAC systems condition bulk indoor dry-bulb temperature and relative humidity, the enclosure separates distinct indoor and outdoor thermodynamic states.

In simplified 1-D modeling, assemblies experience two coupled gradients:

  1. Thermal Gradient: Modeled using steady-state conductive heat transfer principles, where temperature drops across material layers in proportion to each layer's thermal resistance (R-value).
  2. Vapor Pressure Gradient: Modeled using steady-state vapor-diffusion resistance principles, where partial vapor pressure drops across layers in proportion to each material's vapor resistance ($Z = 1/M$).

When the calculated local vapor pressure (P_v) at a material interface equals or exceeds the saturation vapor pressure (P_ws) corresponding to the interface temperature, the simplified steady-state model predicts condensation at that plane.

2. Mathematical Formulations: Conduction, Diffusion & Glaser Method

ASHRAE Hyland-Wexler Saturation Formulation

governing_physics_model.math
ASHRAE / ACCA SPEC
01\ln(p_{ws}) = \frac{C_8}{T} + C_9 + C_{10}T + C_{11}T^2 + C_{12}T^3 + C_{13}\ln(T)
SymbolVariableDescriptionStandard Units
p_{ws}Saturation Vapor PressureSaturation vapor pressure of pure waterpsia
TAbsolute TemperatureThermodynamic dry-bulb temperature°R (°F + 459.67)
C_8..C_{13}Thermodynamic CoefficientsHyland-Wexler coefficients over liquid waterdimensionless

💡 Engineering Note: Reference formulation for moist air psychrometric properties above 32°F (0°C); separate formulation coefficients apply over ice.

🏛️Engineering Standard Reference: ASHRAE Handbook of Fundamentals (Psychrometric formulation over liquid water)

1-D Steady-State Interface Temperature Model

governing_physics_model.math
ASHRAE / ACCA SPEC
01T_i = T_{\text{inside}} - (T_{\text{inside}} - T_{\text{outside}}) \times \frac{\sum_{j=1}^i R_j}{R_{\text{total}}}
SymbolVariableDescriptionStandard Units
T_iInterface TemperatureCalculated temperature at the boundary between layers i and i+1°F
R_jLayer Thermal Resistance1-D thermal resistance of individual layerhr·ft²·°F/Btu
R_{ ext{total}}Total 1-D Assembly R-ValueSeries sum of material layer and air film resistanceshr·ft²·°F/Btu

💡 Engineering Note: Assumes idealized 1-D series heat conduction without accounting for framing thermal bridges, fasteners, or 2D/3D bypasses.

🏛️Engineering Standard Reference: ASHRAE Handbook of Fundamentals (1-D series resistance model)

Steady-State Vapor-Diffusion Resistance Model

governing_physics_model.math
ASHRAE / ACCA SPEC
01P_{v,i} = P_{v,\text{in}} - (P_{v,\text{in}} - P_{v,\text{out}}) \times \frac{\sum_{j=1}^i (1 / M_j)}{\sum_{j=1}^n (1 / M_j)}
SymbolVariableDescriptionStandard Units
P_{v,i}Interface Vapor PressureModeled partial vapor pressure at interface iin.Hg (or psia)
M_jWater Vapor PermeancePerm rating of layer (e.g., tested per ASTM E96 standard methods)US Perms (grain/hr·ft²·in.Hg)
1/M_jVapor Resistance (Rep)Resistance to vapor transmission through layer jRep (hr·ft²·in.Hg/grain)

💡 Engineering Note: Distributes vapor pressure across layers based on diffusion resistance, assuming purely diffusion-driven vapor flow.

🏛️Engineering Standard Reference: ASHRAE Fundamentals Ch. 26 & EN ISO 13788 (Glaser diffusion model)

Glaser Interstitial Condensation Mass Flux (Model Formulation)

governing_physics_model.math
ASHRAE / ACCA SPEC
01g_c = \frac{P_{v,\text{in}} - P_{ws,i}}{Z_{\text{in} \to i}} - \frac{P_{ws,i} - P_{v,\text{out}}}{Z_{i \to \text{out}}}
SymbolVariableDescriptionStandard Units
g_cModeled Condensation RateTheoretical condensation mass flux at condensing interface igrains / (hr·ft²)
P_{ws,i}Saturation Vapor Pressure at PlaneSaturated vapor pressure at interface temperature T_iin.Hg
ZCumulative Vapor ResistanceVapor resistance between boundary and condensing planeRep

💡 Engineering Note: Idealized steady-state calculation; does not account for transient weather, moisture storage (sorption), capillary suction, or air leakage.

🏛️Engineering Standard Reference: EN ISO 13788 & ASHRAE Fundamentals Ch. 26 (Glaser method)

Methodology & Model Limitations (Glaser Method)

The Glaser calculation presented here is a simplified, steady-state, one-dimensional vapor-diffusion model. Key limitations include:

  • Assumes steady-state thermal and vapor boundary conditions rather than dynamic hourly climatic data.
  • Models 1-D vapor diffusion only; does not model bulk air leakage (convective vapor transport), which is often the dominant moisture transport mechanism in field assemblies.
  • Neglects hygrothermal sorption, liquid capillary suction, rain-water intrusion, and material moisture storage capacity.
  • Does not model 2-D or 3-D thermal bridging at structural framing, fasteners, corners, and window interfaces.

3. Hydrothermal Case Study: Cold Climate (Zone 5/6) Winter Steady-State Scenario

To illustrate how the 1-D Glaser method evaluates interface conditions, the table below compares two sample wall configurations under steady-state winter boundary conditions (Indoor: 70°F @ 40% RH, P_v,in ≈ 0.295 in.Hg; Outdoor: 10°F @ 80% RH, P_v,out ≈ 0.051 in.Hg):

Assembly Configuration1-D Assembly R-ValueEvaluated PlaneInterface Temp ($T$)Model Local RHModel Status
Standard 2x6 + R-20 Batt + Kraft (Class II) + OSB~R-23.4OSB sheathing interface~14.4°F100%Condensation Predicted
Continuous ci 2x6 + R-20 Batt + R-7.5 Exterior Continuous (ci)~R-30.9OSB sheathing interface~27.9°F100%No Condensation Predicted (Under Model Assumptions)

Analytical Takeaway: In the standard assembly, the cold sheathing temperature (~14.4°F) lowers the saturation vapor pressure (P_ws ≈ 0.082 in.Hg) below the local vapor pressure (P_v), predicting condensation. Adding R-7.5 continuous exterior insulation (ci) warms the OSB sheathing interface to approximately 27.9°F in this 1-D model, raising the local saturation vapor pressure (P_ws ≈ 0.151 in.Hg). Because local vapor pressure remains below saturation (P_v < P_ws), the model predicts no condensation under these specific steady-state assumptions.

4. Vapor Retarder Classifications (IRC Section R702.7 & Building Standards)

Model building codes (such as the International Residential Code, Section R702.7) categorize vapor retarder materials based on water vapor permeance tested in accordance with standard test methods (such as ASTM E96):

Class I Vapor Impermeable
≤ 0.1 Perm

Sheet polyethylene (e.g., 6-mil poly), unperforated foil, sheet metal. Often referenced for severe heating climates; may limit inward drying in cooling-dominated environments.

Class II Vapor Semi-Impermeable
0.1 < Perm ≤ 1.0

Kraft paper facing on fiberglass batts, smart polyamide variable-permeance membranes, bituminized paper. Frequently used in mixed and cold climate framing.

Class III Vapor Semi-Permeable
1.0 < Perm ≤ 10.0

Latex paint over drywall, fiberboard, plywood. Permitted by IRC provisions under specific climate zones, continuous exterior insulation levels, or ventilated cladding conditions.

5. Inward Solar Vapor Drive Considerations in Warm and Humid Climates

Moisture problems can occur when vapor-control and drying strategies are inappropriate for the climate and wall assembly. In warm, humid, or cooling-dominated climates:

  • Solar Vapor Drive: Rain saturation of porous reservoir claddings (such as brick veneer, stucco, or fiber cement) followed by solar radiation can elevate the moisture vapor pressure behind the cladding.
  • Inward Migration: Vapor moves inward toward the air-conditioned interior space where lower vapor pressures exist.
  • Interior Vapor Retarder Trapping: If an impermeable interior layer (such as sheet poly or impermeable vinyl wall covering) is present on the interior conditioned side, inward-driven vapor can accumulate on the cooled interior surface, elevating moisture content and contributing to mold risk over extended periods.

Design Consideration: Vapor-control strategies in cooling-dominated and mixed climates must account for climate, assembly configuration, moisture sources, drying potential, and applicable code requirements. Interior Class I vapor retarders can require special consideration where inward vapor drive or drying limitations are concerns.

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