Physics for Geologists, Second edition
Physics for Geologists, Second edition
Physics for Geologists, Second edition
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40 Gravity<br />
Figure 3.8 The siphon at rest. The tube joining the two containers of water is<br />
filled with water, providing a continuum from one to the other. The<br />
water in the tube is in tension - at less than atmospheric pressure -<br />
but no water moves because the energy at each end of the tube is the<br />
same.<br />
petrol from one container to another. The physics of this siphon requires<br />
some careful thought. It is easily misunderstood. Let us begin with the two<br />
containers at the same level, with a water-filled tube passing from one to the<br />
other. What is going on here? Clearly nothing. The pressure at the surface<br />
of the water in the containers is atmospheric, whatever that might be. In<br />
the tube connecting the two, the pressure decreases upwards from each con-<br />
tainer and is at a minimum at the crest of the tube. The water here then is<br />
in tension. How high can the tube rise above the levels in the containers and<br />
still maintain continuity of the water in the tube? The limit is the height at<br />
which a vacuum (vapour pressure) will be <strong>for</strong>med at the arch. That is a little<br />
more than 10 m. This is the limit at which water in a well can be raised by<br />
a suction pump at the surface. In general, though, the tube can rise and fall<br />
between the two containers as long as it remains within the limits.<br />
If you were to make a hole in the connecting tube at the crest, the water<br />
would subside on both sides into the containers, and air would be sucked in<br />
through the hole. Likewise, if the wall of the tube is not strong enough, it<br />
would flatten at the crest.<br />
The essential feature of the siphon at rest, as it were, is that the tube<br />
filled with water provides a continuum from one container to the other. The<br />
water in the tube has higher potential energy than that in the containers, but<br />
nothing moves because the potential energies of each side are the same. To<br />
move the water involves work, which requires energy.<br />
If you now raise one of the containers without breaking the continuity<br />
of the water in the tube (Figure 3.9), what changes? The most significant<br />
change is that the potential energy in the higher container becomes greater<br />
than that in the lower. Provided the water is continuous in the tube, the water<br />
flows from the higher to the lower container. It flows from larger pressure to<br />
smaller pressure in the short arm of the tube, and from smaller pressure to<br />
Copyright 2002 by Richard E. Chapman