...vibration, and is therefore (as Plateau shows) proportional cateris paribus to the square root of the head. The time of vibration is of course itself a function...in Appendix II it is proved that its expression is /O~-T7\ (io), V being the volume of the vibrating mass. In an experiment arranged to determine the...

...and is therefore, as Plateau shewed, proportional cceteris paribus to the square root of the head. The time of vibration is of course itself a function of the nature of the fluid (T, p) and of the size of the drop, to the calculation of which we now proceed. It may be remarked...

...and is therefore, as Plateau shewed, proportional cceteris paribus to the square root of the head. The time of vibration is of course itself a function of the nature of the fluid (T, p) and of the size of the drop, to the calculation of which we now proceed. It may be remarked...

...vibratkm,and is there forc( as PlaUau shows) proportional cetera par i bus to the square root of the head. The time of vibration is of course itself a function...inversely as the square root of the capillary tension; and it may be proved that its expression is V being the volume of the vibrating mass. In consequence of...

...Plateau shows) proportional cclirii paribus to the square root of the head. The timeof vibration isof course itself a function of the nature of the fluid and of the size of the drop. By the method of dimen sions alone it may be seen that the time of infinitely small vibrations varies directly as the...