✈️ Standard Atmosphere Calculator (ISA 1976)

Determine U.S. Standard Atmosphere ($ISA$ 1976 / $ISO$ 2533) atmospheric properties at any geometric or pressure altitude. Supports temperature deviations, calculates density altitude, and tracks layers in real-time.

📋 Input Settings

System Units: SI Metric (m, K, Pa, kg/m³)
Adjust Altitude Slider 0 m
Offsets the standard local temperature to evaluate non-standard conditions (Density Altitude, actual density, etc.).

🚀 Core Parameters

Geopotential Height ($h$): 0.00 m
Local standard Temp ($T_{std}$): 15.00 °C
Pressure Altitude ($z_p$): 0.00 m
Density Altitude ($z_d$): 0.00 m

📈 Atmospheric Layer Profile

Tropopause (11 km / FL360) Stratopause (51 km) Mesopause (86 km) 0 km 11 km 20 km 32 km 47 km 51 km 71 km 86 km TROPOSPHERE STRATOSPHERE MESOSPHERE z: 0 m

📊 Calculated Air Properties

Actual Temperature ($T$) 288.15 K
Actual Pressure ($P$) 101,325 Pa
Air Density ($\rho$) 1.2250 kg/m³
Speed of Sound ($a$) 340.29 m/s
Property Name Symbol SI Metric Value Imperial Value
Geometric Altitude z - -
Geopotential Altitude h - -
Temperature (Standard) T_std - -
Temperature (Actual) T - -
Atmospheric Pressure P - -
Density of Air ρ - -
Speed of Sound a - -
Dynamic Viscosity μ - -
Kinematic Viscosity ν - -
Thermal Conductivity k - -
Mean Free Path λ - -
Local Gravity Acceleration g - -
Pressure Altitude z_p - -
Density Altitude z_d - -
Pressure Ratio δ -
Temperature Ratio θ -
Density Ratio σ -

📘 Standard Atmosphere Mathematical Models

1. Geopotential Height & Gravity

The standard model integrates hydrostatic balance on a geopotential height $h$ to simplify the gravity variation $g(z)$ at geometric altitude $z$:

$$h = \frac{r_e \cdot z}{r_e + z}$$ $$g(z) = g_0 \cdot \left(\frac{r_e}{r_e + z}\right)^2$$

Where the nominal Earth radius is $r_e = 6,356,766\text{ m}$, and gravity at sea level is $g_0 = 9.80665\text{ m/s}^2$.

2. Thermal Profile & Pressure

Within any atmospheric layer $b$ characterized by a constant temperature lapse rate $L_b = \frac{dT_{std}}{dh}$:

  • If $L_b \neq 0$ (Linear lapse rate): $$T_{std} = T_b + L_b(h - h_b)$$ $$P = P_b \cdot \left[1 + \frac{L_b(h - h_b)}{T_b}\right]^{-\frac{g_0 M}{R^* L_b}}$$
  • If $L_b = 0$ (Isothermal layer): $$T_{std} = T_b$$ $$P = P_b \cdot \exp\left[-\frac{g_0 M (h - h_b)}{R^* T_b}\right]$$

Where $M = 0.0289644\text{ kg/mol}$ is the molecular weight of air, and $R^* = 8.31432\text{ J/(mol K)}$ is the universal gas constant.

3. Transport & Kinetic Properties

Standard viscosity is governed by Sutherland's law, and thermal conductivity utilizes an empirical formulation:

$$\mu = 1.458 \times 10^{-6} \cdot \frac{T^{1.5}}{T + 110.4}$$ $$k = \frac{2.64638 \times 10^{-3} \cdot T^{1.5}}{T + 245.4 \times 10^{-12 / T}}$$

The mean free path $\lambda$ (average distance traveled between molecular collisions) is computed based on effective collision diameter $d = 3.65\text{ Å}$:

$$\lambda = \frac{k_B T}{\sqrt{2} \pi d^2 P} \approx \frac{2.33228 \times 10^{-5} \cdot T}{P}$$