Analyze acoustic speed using trusted physical relationships. Choose gas, liquid, solid, or direct measurement modes. Get instant results, export reports, and inspect plotted behavior.
| Case | Inputs | Model | Approx. Velocity |
|---|---|---|---|
| Air at 20°C | γ = 1.4, M = 28.97 g/mol, P = 101325 Pa | Gas | 343.2 m/s |
| Fresh water | K = 2.2 GPa, ρ = 998 kg/m³ | Liquid | 1484.8 m/s |
| Steel longitudinal wave | E = 200 GPa, ν = 0.29, ρ = 7850 kg/m³ | Solid | ≈ 5850 m/s |
| Measured pulse | d = 15 m, t = 0.044 s | Direct | 340.9 m/s |
Sound velocity is the speed at which a pressure disturbance moves through a medium. It depends on elasticity, compressibility, density, and temperature.
In gases, warmer molecules transfer pressure disturbances faster. That is why sound speed rises as absolute temperature increases.
Water is much less compressible than air. Although water is denser, its higher resistance to compression usually dominates and produces greater sound speed.
Acoustic impedance equals density multiplied by sound velocity. It helps describe reflection and transmission behavior at material boundaries.
Choose longitudinal for compressional waves traveling along the material. Choose shear for transverse motion in an isotropic solid.
Yes. Enter an optional frequency, and the calculator computes wavelength from velocity divided by frequency.
Use direct mode when you already know the traveled distance and measured time. It is useful for experiments and field measurements.
No. Real materials can be anisotropic, nonlinear, or temperature sensitive. The results are strong estimates when the chosen model matches the medium.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.