Every shape of the liquid surface and every way of transition is related to the surface tension of the liquid, so it can be used to measure the surface tension. There are many methods of determination, and several commonly used methods are listed in Table 4-4.
| test methods | icon | Calculation formula | Features and scope of application |
| capillary rise method | ![]() | γ=ρghr/2cosθ When θ is 0, the correction equation for the hemispherical meniscus is: γ=1/2· ρ(h+1/3)rg | Accurate, simple, slow speed, large amount of liquid; suitable for liquids with a contact angle of 0 |
| Maximum bubble pressure method (dynamic) | ![]() |
| Simple, fast, and convenient for remote control; independent of contact angle, suitable for inaccessible high-temperature liquids, not suitable for aging surfaces |
| Drop Gravimetry | ![]() | γ =Wg/2πrf When r/V 1/3 =0.6~1.2, f≈0.6 | Suitable for very small droplets, and can also be used to measure liquid-liquid interfacial tension |
| circle method | ![]() | γ=(FW ring g)/4πr | Convenient, but requires correction; suitable for liquids with contact angles close to 0 |