Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great BritainFleming, J. A. (John Ambrose), Sir
Science
Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great Britain
Fleming, J. A. (John Ambrose), Sir
Electric waves; Sound; Waves
Mr. Froude’s experiments on this point were very extensive. For
example, he showed that the skin friction of a clean copper surface
such as forms the sheathing of a ship may be taken to be about one
quarter of a pound per square foot of wetted surface when moving at 600
feet a minute. This is equivalent to saying that a surface of 4 square
feet of copper moved through water at the rate of 10 feet a second
experiences a resisting force equal to the weight of 1 lb. due entirely
to skin friction. Very roughly speaking, this skin resistance increases
as the square of the speed.[17] Thus at 20 feet per second the skin
friction of a surface of 4 square feet of copper would be 4 lbs., and
at 30 feet per second it would be 9 lbs. Any roughness of the copper
surface, however, greatly increases the skin friction, and in the case
of a ship the accumulation of barnacles on the copper sheathing has
an immense effect in lowering the speed of the vessel by increasing
the skin friction. Hence the necessity for periodically cleaning the
ship’s bottom by scraping off these clinging growths of seaweed and
barnacles.
Mr. Froude also made many experiments on surfaces of paraffin wax,
because of this material his ship models were made. It may suffice to
say that the skin friction in this case, in fresh water, is such that
a surface of 6 square feet of paraffin wax, moving at a speed of 400
feet per minute, would experience resistance equal to the weight of 1
lb. There are, however, certain corrections which have to be applied
in practice to these rules, depending upon the length of the immersed
surface. The mean speed of the water past the model or ship-surface
depends on the form of the stream-lines next to it, and it has already
been shown that the velocity of the water next to the ship is not the
same at all points of the ship-surface. It is greater near the centre
than at the ends. Hence the longer the model, the less is the mean
resistance per square foot of wetted surface due to skin friction when
the model is moved at some constant speed through the water.
The above explanations will, however, be sufficient to enable the
reader to understand in a general way the problem to be solved in
designing a ship, especially one intended to be moved by steam-power.
Public-domain text, read in full here on John Shaqi.
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