Physics for Geologists, Second edition
Physics for Geologists, Second edition
Physics for Geologists, Second edition
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
112 Fluids and fluid flow<br />
Figure 12.1 Speed of non-turbulent flowing water at the surface in a channel<br />
(in plan). The vertical profile is similar to the bottom half of this<br />
diagram.<br />
the viscosity of the water, provide the retarding <strong>for</strong>ces; and when these <strong>for</strong>ces<br />
have reached equilibrium, the water will have constant velocity - constant<br />
on all scales above the molecular if the flow is laminar, only in a gross sense<br />
if it is turbulent. The resistance at the sides means that there will be a velocity<br />
pattern in the surface water, with the greatest velocity at the centre, least at<br />
the sides, decreasing to zero in contact with the sides at what is called the<br />
wetted surface (Figure 12.1). Similarly, there is a vertical velocity profile,<br />
from zero in contact with the base, to a maximum near the surface (why<br />
near, not at? Because there is air resistance to flow at the surface - less,<br />
certainly, than at the sides and bottom, but nevertheless a resistance).<br />
What then do we mean by velocity of a water stream when it is different in<br />
different positions in the water? In laminar flow we can say that the velocity is<br />
constant in any one position in the channel, but the variation of velocity with<br />
position means that we must define velocity of the channel water as a whole<br />
as the volumetric rate of flow divided by the normal cross-sectional area.<br />
Dimensionally that is L3~-l/L2<br />
= LT-l. In units, it is m3 s-I m-2 -<br />
- ms-I.<br />
Wind velocity also has a profile. That is why the stipulated height of<br />
anemometers is 10 m above the ground.<br />
Capillarity<br />
The water of a fountain breaks up into drops that are nearly spherical; a tap<br />
drips drops that are nearly spherical; gas bubbles in soda water are nearly<br />
spherical, and you can remove a fly from water by dipping your finger on<br />
the fly and it is retained in the drop of water you extract. Some insects can<br />
walk on water, and if you look at them carefully you will see that their feet<br />
depress the surface slightly. You can fill a glass with water above the level<br />
of the rim. Capillarity is involved in all these things, and in the underground<br />
fluids, water, crude oil and gas. Soils retain moisture because of capillarity;<br />
crude oil and natural gas reservoirs retain water because of capillarity.<br />
Copyright 2002 by Richard E. Chapman