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Drop weight method

Harkins and Jordan [43] found, however, that Eq. 11-26 was generally in serious error and worked out an empirical correction factor in much the same way as was done for the drop weight method. Here, however, there is one additional variable so that the correction factor/ now depends on two dimensionless ratios. Thus... [Pg.21]

The surface tension of a liquid is determined by the drop weight method. Using a tip whose outside diameter is 5 x 10 m and whose inside diameter is 2.5 x 10 m, it is found that the weight of 20 drops is 7 x 10 kg. The density of the liquid is 982.4 kg/m, and it wets the tip. Using r/V /, determine the appropriate correction factor and calculate the surface tension of this liquid. [Pg.41]

The following values for the surface tension of a 10 Af solution of sodium oleate at 25°C are reported by various authors (a) by the capillary rise method, y - 43 mN/m (b) by the drop weight method, 7 = 50 mN/m and (c) by the sessile drop method, 7 = 40 mN/m. Explain how these discrepancies might arise. Which value should be the most reliable and why ... [Pg.41]

The same system has been studied previously by Boguslavsky et al. [29], who also used the drop weight method. While qualitatively the same behavior was observed over the broad concentration range up to the solubility limit, the data were fitted to a Frumkin isotherm, i.e., the ions were supposed to be specifically adsorbed as the interfacial ion pair [29]. The equation of the Frumkin-type isotherm was derived by Krylov et al. [31], on assuming that the electrolyte concentration in each phase is high, so that the potential difference across the diffuse double layer can be neglected. [Pg.425]

Drop weight method (can also be used for high pressure and temperature)... [Pg.37]

The slow formation of a drop at a submerged circular orifice or nozzle will result in a drop size, predicted by equations for determining interfacial tension by the drop-weight method. At the instant a slowly forming drop breaks away from a nozzle, the force balance may be written... [Pg.54]

Many modifications of the drop weight method have been utilised in practice. [Pg.15]

As we shall have occasion to note in dealing with solutions, the composition of the surface phase is very different from that of the bulk liquid. When a liquid interface is newly formed the system is unstable until the surface phase has acquired its correct excess or deficit of solute by diffusion from or into the bulk of the solution. This process of diffusion is by no means instantaneous and, as has been observed in discussing the drop weight method, several minutes may elapse before equilibrium is established. In the ripple method the surfece is not renewed instantaneously but may be regarded as undergoing a series of expansions and contractions, thus we should anticipate that the value of the surface tension of a solution determined by this method would lie between those determined by the static and an ideal dynamic method respectively. [Pg.17]

Goard has determined the surface tensions of a few salt solutions hy the drop weight method employing the method of Iredale for calculating the surface tension, the following values were obtained. [Pg.55]

The surface tension of mercury in the presence of the vapour at various partial pressures was measured by the drop weight method. The following values were obtained for the surface tensions of mercury in the presence of vapours of methyl acetate, water and benzene at various partial pressures at 26 —27° C. [Pg.57]

OP) J. McCormack et al, "A New Procedure for the Estimation of the Impact Sensitiveness of Explosives , Explosivstoffe 17(10), 225—28(1969). Abstracted in Expls Pyrots 3(8), 1970 (Measurement of the Figure of In sensitiveness for relatively insensitive expls by the drop weight method is improved by detecting gas evolved in "no-fires" with starch-iodide impregnated filter paper. Quantities of gas less than 1 cc are readily detected)... [Pg.353]

Impact Sensitivity. Values determined by the drop weight method have the usual dependence... [Pg.741]

There are numerous other methods for measuring surface tension that we do not discuss here. These include (a) the measurement of the maximum pressure beyond which an inert gas bubble formed at the tip of a capillary immersed in a liquid breaks away from the tip (the so-called maximum bubble-pressure method) (b) the so-called drop-weight method, in which drops of a liquid (in a gas or in another liquid) formed at the tip of a capillary are collected and weighed and (c) the ring method, in which the force required to detach a ring or a loop of wire is measured. In all these cases, the measured quantities can be related to the surface tension of the liquid through simple equations. The basic concepts involved in these methods do not differ significantly from what we cover in this chapter. The experimental details may be obtained from Adamson (1990). [Pg.255]

Several additional points might be noted about the use of the Bashforth-Adams tables to evaluate 7. If interpolation is necessary to arrive at the proper (3 value, then interpolation will also be necessary to determine (x/bl. . This results in some loss of accuracy. With pendant drops or sessile bubbles (i.e., negative /3 values), it is difficult to measure the maximum radius since the curvature is least along the equator of such drops (see Figure 6.15b). The Bashforth-Adams tables have been rearranged to facilitate their use for pendant drops. The interested reader will find tables adapted for pendant drops in the material by Padday (1969). The pendant drop method utilizes an equilibrium drop attached to a support and should not be confused with the drop weight method, which involves drop detachment. [Pg.283]

Drop-weight method. Here, the liquid is allowed to flow out from the bottom of a capillary tube. Drops are formed which detach when they reach a critical dimension. The weight of a drop falling out of a capillary is measured. To get a precise measure, this is done for a number of drops and the total weight is divided by this number. [Pg.13]

Figure 2.9 Maximal bubble pressure and drop-weight method to measure the surface tension of liquids. Figure 2.9 Maximal bubble pressure and drop-weight method to measure the surface tension of liquids.
Drop-weight method. To determine the surface tension of a hexadecane (Ci6H34) you let it drop out of a capillary with 4 mm outer and 40 /. m inner diameter. Hexadecane wets the capillary. Its density is 773 kg/m3. 100 drops weigh 2.2 g. Calculate the surface tension of hexadecane using the simple Eq. (2.15) and the correction factor /. It was concluded that / should be a function of rc/V 1/3, with V being the volume of the drop. Values for the correction factor are listed in the following table (from Ref. [1], p. 19). Is it necessary to use the correction ... [Pg.24]

Drop-weight method. With a mass m = 2.2 x 10 3kg/100 volume of one drop is... [Pg.300]

Figure 4.8 Correction factor for drop volume and drop weight methods... Figure 4.8 Correction factor for drop volume and drop weight methods...
Harkins and his colleagues1 have extended these measurements of the work of adhesion to water, and also to mercury.2 The measurements of surface tension were made by the drop-weight method, using the corrections necessary for accurate results as three separate measurements of surface tension are required, considerable accuracy is desirable for trustworthy results in the work of adhesion. [Pg.154]

There are static and dynamic methods. The static methods measure the tension of practically stationary surfaces which have been formed for an appreciable time, and depend on one of two principles. The most accurate depend on the pressure difference set up on the two sides of a curved surface possessing surface tension (Chap. I, 10), and are often only devices for the determination of hydrostatic pressure at a prescribed curvature of the liquid these include the capillary height method, with its numerous variants, the maximum bubble pressure method, the drop-weight method, and the method of sessile drops. The second principle, less accurate, but very often convenient because of its rapidity, is the formation of a film of the liquid and its extension by means of a support caused to adhere to the liquid temporarily methods in this class include the detachment of a ring or plate from the surface of any liquid, and the measurement of the tension of soap solutions by extending a film. [Pg.363]

For rapid work, requiring an accuracy of about three-tenths per cent., Sugden s modification of the maximum bubble-pressure method is probably the most convenient very little apparatus is required, and a complete measurement can easily be made in 15 minutes. Two or three cubic centimetres of the liquid are all that is necessary. The drop-weight method (using Harkins s indispensable corrections) is also simple and equally accurate. [Pg.388]

Drop time method - drop weight method... [Pg.170]

For measurement of interfacial tension see also -> Wilhelmy plate (slide) method, -> drop weight method, -> ring method. There are also a number of other static and dynamic methods for the determination the interfacial tension [viii]. [Pg.361]

For measurement of interfacial tension see also - Wilhelmy plate (slide) method, - drop weight method,... [Pg.405]


See other pages where Drop weight method is mentioned: [Pg.19]    [Pg.43]    [Pg.454]    [Pg.38]    [Pg.8]    [Pg.12]    [Pg.13]    [Pg.15]    [Pg.18]    [Pg.41]    [Pg.325]    [Pg.14]    [Pg.386]    [Pg.74]    [Pg.377]    [Pg.379]    [Pg.387]    [Pg.170]    [Pg.185]    [Pg.309]   
See also in sourсe #XX -- [ Pg.13 , Pg.24 ]

See also in sourсe #XX -- [ Pg.1117 ]




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