1. Longitudinal Wave Speed
- Range: Approximately 5,700–5,900 m/s (Slight variations occur due to differences in alloy composition; e.g., 304 stainless steel ≈ 5,790 m/s)
2. Shear Wave Speed
- Range: Approximately 3,100–3,200 m/s (Shear wave speed is typically 50–60% of the longitudinal wave speed)
Factors Affecting Sound Speed
-
Material Composition:
- The proportions of alloying elements (e.g., chromium (Cr), nickel (Ni)) influence density and elastic modulus, thus altering sound speed.
- For example, 316 stainless steel (containing molybdenum (Mo)) may have a slightly lower sound speed than 304.
-
Temperature:
- Sound speed decreases slightly with rising temperature (due to thermal expansion affecting material density).
-
Pipe Processing Condition:
- Cold working (e.g., cold rolling) may introduce internal stresses, causing minor variations in sound speed.

Practical Applications
- Ultrasonic Testing (UT): In industrial inspections, the sound speed must be calibrated for the specific stainless steel grade to ensure accurate defect detection.
- Acoustic Design: If used in sound transmission applications (e.g., medical devices or sensors), the relationship between sound speed and frequency must be considered.
Reference Data
| Stainless Steel Grade | Longitudinal Wave Speed (m/s) | Shear Wave Speed (m/s) |
|---|---|---|
| 304 Stainless Steel | ~5,790 | ~3,100 |
| 316 Stainless Steel | ~5,740 | ~3,080 |
For precise values, experimental measurement or calculation using the elastic modulus (E) and Poisson’s ratio (ν) is recommended: Longitudinal Wave Speed=E(1−ν)ρ(1+ν)(1−2ν)Longitudinal Wave Speed=ρ(1+ν)(1−2ν)E(1−ν) (where ρ = density; e.g., 304 stainless steel ≈ 7,930 kg/m³)
Note: Under extreme conditions (e.g., high temperature/pressure), corrections based on actual environmental parameters may be necessary.

