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diaphragm viton fkm
Elastomeric Teflon Diaphragms Rubber to metal bonding in diaphragm manufacturing. Fabric reinforced diaphragms Homogenous diaphragms Fab•Air Specialty Industrial Diaphragms
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Dia•Com is a leading international provider of innovative, cost-effective molded diaphragm solutions critical to the operation of essential systems and equipment in industrial, automotive, aerospace, medical instrumentation, and food and water processing applications. The company's reputation for excellence is based on superior quality in the design, manufacture and application of its high-performance, state-of-the-art, fabric-reinforced and homogeneous elastomeric diaphragm seals.

Polymers are a diverse category of materials characterized by chains of covalently-bonded atoms with repeating structural units. The materials can be processed in numerous ways with almost infinite variation. The properties of polymers are determined by a number of factors including crystallinity, density, chain orientation, cross-linking, purity, phase distribution, etc. We are unaware of hydrogen compatibility studies for common polymer materials that might be expected in gaseous hydrogen service, thus we have eliminated the sections on mechanical properties and microstructural considerations. Gas permeation through polymer materials, however, has been extensively studied; therefore we provide a non-exhaustive summary of hydrogen transport data in common polymer materials. Relatively large amounts of hydrogen are often soluble in polymer materials; therefore, exposure to high-pressure hydrogen may cause damage (blistering or swelling) of the polymer materials. This is manifest in high-pressure applications due to depressurization of a system (or rapid temperature changes) as hydrogen expands in free volume and at interfaces within the polymers. . 1.1 Composition and microstructure Polymers are generally characterized by the composition and molecular structure of the material. Nomenclature often evolves from common usage and generally does not incorporate structural details. We use ASTM D1418 and D1600 for guidance on naming. Table 1.1.1 includes the abbreviations used in this document. 2. Permeability, Diffusivity and Solubility Hydrogen transport in polymers has been extensively studied, particularly for high-vacuum systems. Similar to studies of metals, studies of the hydrogen permeation in polymers have generally been performed at low pressure. Permeability, diffusivity and solubility are often assumed to be independent of pressure for metals and data generated at low-pressure are extrapolated to describe high-pressure systems. This extrapolation implies that hydrogen transport and solubility properties are independent of concentration (i.e., Fickian diffusion). While concentration-dependent transport properties (non-Fickian diffusion) are often observed in polymers, we are unaware of any studies on polymers that suggest hydrogen transport and solubility are dependent on concentration. Thus, until studies show otherwise, we assume that hydrogen permeability, diffusivity and solubility in polymers are independent of pressure. Unlike metals, hydrogen transport in polymer materials is sufficiently rapid that the permeation rates can generally be measured at or near ambient temperature. Nonmetals Polymers 8100 - 2 The permeability (Φ) is determined from Fick's first law for diffusion, and represents a steady-state property of the material (assuming diffusion is independent of pressure). It is defined in the same way as for metals, such that ! " = DS (1) where D is the diffusivity and S is the solubility. Hydrogen transport in polymers differs from metals in one important aspect: hydrogen does not dissociate prior to dissolution in the material, thus the concentration of hydrogen dissolved in the polymer (c) is proportional to the fugacity (f, which equals the pressure in the limit of an ideal gas): ! S = c f (2) while in metals c is proportional to ! f . In materials where hydrogen does not dissociate, such as polymers, it should be clear from equations 1 and 2 that the units of permeability are ! ["] = [diffusivity] [concentration] [pressure] = m2 s mole H 2 m3 MPa = mole H 2 m# s # MPa (3) Other forms of these units are, of course, possible and they can be a significant source of confusion. The units in equation 3 are commonly accepted for high-pressure hydrogen since they do not require definition of a reference state. In tables 2.1 through 2.4, the hydrogen transport properties for a number of polymeric materials are summarized. A secondary resource [1] is used for these values and no effort was made to verify the primary references; the interested reader is also referred to Ref. [2], which contains a lists of primary sources by material. A selection of the hydrogen transport data from Ref. [1] is summarized here. Table 2.1 provides hydrogen transport properties for several common categories of plastics at approximately room temperature. Table 2.2 provides the transport properties for several commercial elastomers near room temperature, while Table 2.3 provides properties for a number of elastomers (rubbers) from a range of classes at room temperature and, when available, at elevated temperature. Permeability, diffusivity and solubility follow a classic exponential form: ! A = A 0 exp "E A RT # $ % & ' ( (4) where A0 and EA are material-dependent constants, R is are the universal gas constant (8.31447 J mol-1 K-1) and T is temperature in Kelvin. Table 2.4 provides the constants from equation 4 that summarize the temperature dependence of these properties for several of the materials from the previous tables. The temperature dependence of hydrogen transport and solubility for the materials in Table 2.4 is plotted in Figure 2.1 (permeability), Figure 2.2 (diffusivity) and Figure 2.3 (solubility); these properties are linear when plotted on a log scale as a function of 1/T as shown in these figures.

 

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