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Explore the theoretical underpinnings of fluid coupling operation in mechanical power transmission systems, elucidating concepts such as torque multiplication, viscous shear forces, and the role of fluid viscosity in achieving smooth and efficient power transfer between rotating shafts.

Sagot :

Answer: write this

Explanation:

The most fundamental approach for analysing the mechanical behaviour of a fluidic

system may be a ‘deterministic’ molecular approach in which the dynamics of individual molecules is investigated by writing their respective equations of motion.

While this is fundamentally appealing and may be suitable for certain cases, several

practical constraints also seem to be inevitable. In order to appreciate the underlying

consequences, consider the molar volume of a gas at normal temperature and pressure, which, by Avogadro’s hypothesis, contains 6.023 ¥ 1023 number of molecules.

To describe motion of each of these molecules, three translational velocity components (along three mutually perpendicular coordinate directions) and three rotational

components (along the same coordinate directions as above) need to be specified.

Therefore, one has to deal with 6 ¥ 6.023 ¥ 1023 number of equations of motion, even

for an elementary molar volume, which is an extremely demanding computational task

even today, in spite of the advent of high-speed supercomputers. Hence, from a

practical point of view, there must be certain approaches that can reduce the number

of variables to a figure that can be handled conveniently for practical computations.

In particular, there are two specific approaches that can be introduced in this

context. In one approach, we deal with ‘statistically averaged’ behaviour of many

molecules constituting the matter under investigation. This is exactly the approach

followed in kinetic theories of matter and statistical mechanics, which in general is

termed as the ‘microscopic’ point of view, since the primary focus of attention is on

the averaged behaviour of individual microscopic constituents of matter.

The second approach reduces the number of variables even further, by considering the gross effect of many molecules that can be captured by direct measuring

instruments and can be perceived by our senses. Such an approach is the so-called

‘macroscopic’ approach. For a clearer distinction between macroscopic and microscopic approaches, we can refer to a very simple example as follows: When we conceive the term ‘pressure’ of a gas (we will deal with this term more formally later) in the

microscopic point of view, it originates out of the rate of change of momentum of

molecules as a consequence of a collision. On the other hand, from a macroscopic

point of view, we describe the same quantity in terms of time-averaged force over a

given area, which can be measured by a pressure gauge.

Though the macroscopic approach provides us with a more practical method of

analysis, one should not presume that it can give the correct solution in all situations.

In order to assess the underlying implications, let us consider certain aggregations of

molecules, such as a set of widely spaced molecules for a gas and a set of closely

spaced molecules for a liquid. If we consider a very small elementary volume within

the medium, then numerous molecules may come into it or move out of it during some