How the wall thermal design is made
A thermal design checks that an external wall does not lose too much heat and that its inner surface does not get cold enough to collect moisture. The Russian code is SP 50.13330 «Thermal performance of buildings». The main quantity is the resistance to heat transfer R₀ (m²·°C/W): the larger it is, the warmer the wall. For a multilayer wall R₀ = 1/α_int + Σδᵢ/λᵢ + 1/α_ext with α_int = 8.7 W/(m²·°C) on the inner surface and α_ext = 23 W/(m²·°C) on the outer one.
Required resistance by degree-days
The norm depends on the climate through the degree-days of the heating period: D_d = (t_int − t_ht)·z_ht, where t_int is the indoor temperature, t_ht and z_ht are the mean temperature and the length of the heating period (the period with a mean daily temperature of at most 8 °C, and at most 10 °C for children and medical buildings). The base value comes from table 3 of SP 50: R_base = a·D_d + b. For walls of dwellings a = 0.00035 and b = 1.4, for public buildings a = 0.0003 and b = 1.2, for industrial buildings with a dry regime a = 0.0002 and b = 1.0. For example, for Moscow D_d = (20 + 2.2)·205 = 4551 °C·day and R_base = 0.00035·4551 + 1.4 = 2.99 m²·°C/W.
The sanitary requirement and the dew point
Besides energy saving, the sanitary requirement is checked: the difference between the air and the inner surface Δt = (t_int − t_ext)/(R₀·α_int) must not exceed the normative Δt_n (4.0 °C for walls of dwellings), and the temperature of the inner surface must be above the dew point of the indoor air. If the surface is colder than the dew point, condensate forms on the wall and mould appears. The page finds the dew point from the air temperature and relative humidity (ASHRAE formulas, as on the i-d chart).
Insulation thickness
If you pick the layer whose thickness is needed, the calculator subtracts the resistance of the other layers and of the surfaces from the required one and divides the remainder by the conductivity of the insulation. The result is rounded up to 10 mm. The factor r accounts for thermal non-uniformity (fasteners, reveals, joints): the reduced resistance is r·R₀.
Condensation inside the wall
A simplified check by the Glaser method: the vapour pressure falls from the inside to the outside in proportion to the vapour resistance of the layers δ/μ, and the temperature changes linearly within a layer. Where the vapour pressure exceeds the saturation pressure at the temperature of the layer, condensate is possible. The dangerous zone usually lies at the boundary of a warm dense layer and the insulation, on the side of the outer layers. Insulation outside and a vapour barrier inside lower the risk. The method ignores sorption, air flow and the yearly cycle, so it is approximate.
Limitations
The calculation assumes a one-dimensional flow through a flat wall. Windows, thermal bridges, junctions and the ground need separate calculations. The data are for reference: before using them in a design, check them against the editions of SP 50.13330 and SP 131.13330 in force.