By H.A. Barnes

ISBN-10: 0444871403

ISBN-13: 9780444871404

Rheology is, by means of universal consent, a tough topic and a few of the theoretical elements are usually seen as being of prohibitive complexity through scientists with no powerful mathematical heritage. There also are the problems inherent in any multidisciplinary technology like rheology for people with a particular education. hence, newbies to the sector are often discouraged, and for them the present texts at the topic - a few of that are amazing - are of restricted counsel as a result of their intensity of element and hugely mathematical nature.This booklet introduces the topic of rheology in phrases comprehensible to non-experts and describes the applying of rheological ideas to many commercial items and procedures. It offers an easy yet authoritative advisor which exhibits in actual fact how arithmetic, physics and chemistry have contributed to the improvement of rheology. The general beneficial properties of all liquid-like fabrics are summarised, i.e. viscosity, linear viscoelasticity, basic stresses and extensional viscosity. specific structures are then mentioned, i.e. polymeric beverages and suspensions. the ultimate bankruptcy provides an summary of the theoretical advances which were made. constant notation and nomenclature were used through the e-book, and the foremost textbooks and courses so one can permit the reader to persist with up specific themes are indexed.

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**Extra resources for An Introduction to Rheology**

**Example text**

E. e. an element in which the force is porportional to the rate of extension) as shown in Fig. 2. 4) (with P, = q ) , respectively. The behaviour of more complicated materials is described by connecting the basic elements in series or in parallel. The Kelvin model results from a parallel combination of a spring and a dashpot (Fig. 3(a)). A requirement on the interpretation of this and all similar diagrams is that the horizontal connectors remain parallel at all times. Hence the extension (strain) in the spring is at all times equal to the extension (strain) in the dashpot.

In the experimental conditions of small-amplitude oscillatory shear, in which linear viscoelasticity is demonstrated and the parameters measured, the three normal stress components have the same value. They are equal to the ambient pressure, which is isotropic. Similarly, in steady flow conditions, provided the flow is slow enough for second-order terms in j. to be negligible, the normal stresses are + Normal stresses 56 [Chap. 4 again equal to the ambient pressure. As the shear rate is increased, the normal stress differences first appear as second-order effects, so that we can write where A , and B, are constants and, as implied, the normal stress differences are even functions of the shear rate p.

6). 5): From this equation we see the effect of changes in such variables as pipe radius. For Newtonian liquids, the pressure drop for a given flow rate is proportional to the fourth power of the radius, but thls is changed if the liquid is shear-thinning. For instance, if n = f, the pressure drop is proportional to the square of the radius. This is clearly important in any scale-up of pipe flow from pilot plant to factory operation. Viscosity [Chap. 2 Fig. 15. The velocity profiles for the laminar flow of power-law liquids in a straight circular pipe, calculated for the same volumetric throughput.