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Differential tension

As a package increases in diameter, the tension will build up and deform the package, hence a device known as a differential tension and pressure attachment (dancing arm) is used... [Pg.411]

Figure 5. Illustration of the Gihhs-Marangoni effect in a thin liquid film. Reaction of a liquid film to a surface disturbance, (a) Low surfactant concentration yields only low differential tension in film. The thin film is poorly stabilized, (b) Intermediate surfactant concentration yields a strong Gibbs-Marangoni effect which restores the film to its original thickness. The thin film is stabilized, (c) High surfactant concentration (> cmc) yields a differential tension which relaxes too quickly due to diffusion of surfactant. The thinner film is easily ruptured. (From Pugh [109]. Copyright 1996 Elsevier, Amsterdam.)... Figure 5. Illustration of the Gihhs-Marangoni effect in a thin liquid film. Reaction of a liquid film to a surface disturbance, (a) Low surfactant concentration yields only low differential tension in film. The thin film is poorly stabilized, (b) Intermediate surfactant concentration yields a strong Gibbs-Marangoni effect which restores the film to its original thickness. The thin film is stabilized, (c) High surfactant concentration (> cmc) yields a differential tension which relaxes too quickly due to diffusion of surfactant. The thinner film is easily ruptured. (From Pugh [109]. Copyright 1996 Elsevier, Amsterdam.)...
Surface tension arises at a fluid to fluid interface as a result of the unequal attraction between molecules of the same fluid and the adjacent fluid. For example, the molecules of water in a water droplet surrounded by air have a larger attraction to each other than to the adjacent air molecules. The imbalance of forces creates an inward pull which causes the droplet to become spherical, as the droplet minimises its surface area. A surface tension exists at the interface of the water and air, and a pressure differential exists between the water phase and the air. The pressure on the water side is greater due to the net inward forces... [Pg.120]

The variation of the integral capacity with E is illustrated in Fig. V-12, as determined both by surface tension and by direct capacitance measurements the agreement confrrms the general correctness of the thermodynamic relationships. The differential capacity C shows a general decrease as E is made more negative but may include maxima and minima the case of nonelectrolytes is mentioned in the next subsection. [Pg.200]

An important part of solving any differential equation is the specification of the boundary conditions. In the present case these can correspond to tension or shear and can be solved to give either a modulus or a compliance. [Pg.187]

Foxboro s Model 823 transmitter uses a taut wire stretched between a measuring diaphragm and a restraining element. The differential process pressure across the measuring diaphragm increases the tension on the wire, thus changing the wire s natural frequency when it is excited by an electromagnet. This vibration (1800—3000 H2) is picked up inductively in an oscillator circuit which feeds a frequency-to-current converter to get a 4—20 m A d-c output. [Pg.213]

Antisymmetric cross-ply laminates were found in Section 4.3.3 to have extensional stiffnesses A, A. 2, A22 = A.. , and Age, bending-ex-tension coupling stiffnesses and B22 = -Bi., and bending stiffnesses Di2. D22 = l ii- Dgg. The new terms here in comparison to a specially orthotropic laminate are and 622- Because of this bending-extension coupling, the three vibration differential equations are coupled ... [Pg.318]

ATBN - amine terminated nitrile rubber X - Flory Huggins interaction parameter CPE - carboxylated polyethylene d - width at half height of the copolymer profile given by Kuhn statistical segment length DMAE - dimethyl amino ethanol r - interfacial tension reduction d - particle size reduction DSC - differential scanning calorimetry EMA - ethylene methyl acrylate copolymer ENR - epoxidized natural rubber EOR - ethylene olefin rubber EPDM - ethylene propylene diene monomer EPM - ethylene propylene monomer rubber EPR - ethylene propylene rubber EPR-g-SA - succinic anhydride grafted ethylene propylene rubber... [Pg.682]

Calculate the maximum value of a rotary torque that may be applied to the drill pipe as specified in Example 5 if the actual working tension load P = 300,000 lb. (For instance, pulling and trying to rotate a differentially stuck drill string.)... [Pg.745]

The more highly charged the interface becomes, the more the charges repel each other, thereby decreasing the cohesive forces, lowering the surface tension, and flattening the mercury drop. The second differential of the electrocapillary plot gives directly the differential capacitance of the double layer ... [Pg.23]

Various methods have been employed for the determination of E of liquid and solid metals. Besides purely electrochemical ones (e.g. measurement of the differential double layer capacity (see also chapter 4.2)) further techniques have been used for the investigation of the surface tension at the solid/electrolyte solution phase boundary. The employed methods can be grouped into several families based on the meas-... [Pg.180]

Measurement of the differential capacitance C = d /dE of the electrode/solution interface as a function of the electrode potential E results in a curve representing the influence of E on the value of C. The curves show an absolute minimum at E indicating a maximum in the effective thickness of the double layer as assumed in the simple model of a condenser [39Fru]. C is related to the electrocapillary curve and the surface tension according to C = d y/dE. Certain conditions have to be met in order to allow the measured capacity of the electrochemical double to be identified with the differential capacity (see [69Per]). In dilute electrolyte solutions this is generally the case. [Pg.183]


See other pages where Differential tension is mentioned: [Pg.2487]    [Pg.69]    [Pg.85]    [Pg.364]    [Pg.2242]    [Pg.179]    [Pg.331]    [Pg.2491]    [Pg.236]    [Pg.125]    [Pg.268]    [Pg.236]    [Pg.294]    [Pg.112]    [Pg.2487]    [Pg.69]    [Pg.85]    [Pg.364]    [Pg.2242]    [Pg.179]    [Pg.331]    [Pg.2491]    [Pg.236]    [Pg.125]    [Pg.268]    [Pg.236]    [Pg.294]    [Pg.112]    [Pg.122]    [Pg.2592]    [Pg.2767]    [Pg.141]    [Pg.34]    [Pg.332]    [Pg.255]    [Pg.308]    [Pg.346]    [Pg.346]    [Pg.346]    [Pg.352]    [Pg.248]    [Pg.1070]    [Pg.1417]    [Pg.1802]    [Pg.280]    [Pg.771]    [Pg.278]    [Pg.26]    [Pg.182]    [Pg.183]   
See also in sourсe #XX -- [ Pg.69 ]




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Constitutive Equations in Differential Form for Multiaxial Tension States

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