Mechanical properties glass transition temperature

Good thermo-mechanical properties. Glass transition temperatures range from 300 to 340 °C. Thermal stability is good up to 400 °C. Elongation to break is typically 20%. On wafer stress is 18 MPa, less than half that found for typical polyimides. 

In this study we showed initial results on the mechanical properties, glass transition temperature and crystallinity of polypropylene+PIB-grafted fumed silica composites. We found that PIB oligomers of different molecular weight on silica have distinct properties in PP. 

The influence of the chemical structure of substances in PMB molecules in the curing process of epoxy materials was investigated. Stress-strain properties were determined by traditional physical-mechanical methods. Glass transition temperature was estimated by the thermomechanical method. Chemical resistance of the epoxy based coating cured by PMBs was determined by change of their impact strength after exposition in an aggressive environment within 42 days. 

The chemical composition of the fibres, their geometry and the spinning conditions define the range of properties glass transition temperature, melting point, heat stability, combustibility, specific electrical resistance, resistance to environment (humidity, chemical, biological, radiation), dye-ability, solubility and the mechanical properties which are listed in the following chapter. The main characteristics of fibres are listed below. 

The method of irradiation and the dose can influence several properties such as thermal properties (glass transition temperature decomposition temperature T(jeo crystallization temperature Tc, and melting temperature T ) and mechanical properties (tensile strength, modulus at 50% elongation, gel... 

Glass Transition. The glass-transition temperature T reflects the mechanical properties of polymers over a specified temperature range. 

Molecular Weight. The values of the mechanical properties of polymers increase as the molecular weight increases. However, beyond some critical molecular weight, often about 100,000 to 200,000 for amorphous polymers, the increase in property values is slight and levels off asymptotically. As an example, the glass-transition temperature of a polymer usually follows the relationship... 

Relatively few processible polyimides, particularly at a reasonable cost and iu rehable supply, are available commercially. Users of polyimides may have to produce iutractable polyimides by themselves in situ according to methods discussed earlier, or synthesize polyimides of unique compositions iu order to meet property requirements such as thermal and thermoxidative stabilities, mechanical and electrical properties, physical properties such as glass-transition temperature, crystalline melting temperature, density, solubility, optical properties, etc. It is, therefore, essential to thoroughly understand the stmcture—property relationships of polyimide systems, and excellent review articles are available (1—5,92). 

Thermal Properties. Spider dragline silk was thermally stable to about 230°C based on thermal gravimetric analysis (tga) (33). Two thermal transitions were observed by dynamic mechanical analysis (dma), one at —75° C, presumed to represent localized mobiUty in the noncrystalline regions of the silk fiber, and the other at 210°C, indicative of a partial melt or a glass transition. Data from thermal studies on B. mori silkworm cocoon silk indicate a glass-transition temperature, T, of 175°C and stability to around 250°C (37). The T for wild silkworm cocoon silks were slightly higher, from 160 to 210°C. 

The dynamic mechanical properties of VDC—VC copolymers have been studied in detail. The incorporation of VC units in the polymer results in a drop in dynamic modulus because of the reduction in crystallinity. However, the glass-transition temperature is raised therefore, the softening effect observed at room temperature is accompanied by increased brittleness at lower temperatures. These copolymers are normally plasticized in order to avoid this. Small amounts of plasticizer (2—10 wt %) depress T significantly without loss of strength at room temperature. At higher levels of VC, the T of the copolymer is above room temperature and the modulus rises again. A minimum in modulus or maximum in softness is usually observed in copolymers in which T is above room temperature. A thermomechanical analysis of VDC—AN (acrylonitrile) and VDC—MMA (methyl methacrylate) copolymer systems shows a minimum in softening point at 79.4 and 68.1 mol % VDC, respectively (86). 

Tackifying resins enhance the adhesion of non-polar elastomers by improving wettability, increasing polarity and altering the viscoelastic properties. Dahlquist [31 ] established the first evidence of the modification of the viscoelastic properties of an elastomer by adding resins, and demonstrated that the performance of pressure-sensitive adhesives was related to the creep compliance. Later, Aubrey and Sherriff [32] demonstrated that a relationship between peel strength and viscoelasticity in natural rubber-low molecular resins blends existed. Class and Chu [33] used the dynamic mechanical measurements to demonstrate that compatible resins with an elastomer produced a decrease in the elastic modulus at room temperature and an increase in the tan <5 peak (which indicated the glass transition temperature of the resin-elastomer blend). Resins which are incompatible with an elastomer caused an increase in the elastic modulus at room temperature and showed two distinct maxima in the tan <5 curve. 

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