At infinity U = -me a cos (i = a m b oos (3, V= -me a sin 1 3 - C7,1 sin 0, (9) a and b denoting the semi-axes of the ellipse a; so that the liquid is streaming at infinity with velocity Q = m/(a+b) in the direction of the **asymptote** of the hyperbola (3.

A relation which is of historical interest connects the logarithmic function with the quadrature of the hyperbola, for, by considering the equation of the hyperbola in the form xy=const., it is evident that the area included between the arc of a hyperbola, its nearest **asymptote**, and two ordinates drawn parallel to the other **asymptote** from points on the first **asymptote** distant a and b from their point of intersection, is proportional to log bla.

The area of the loop, which equals the area between the curve and its **asymptote**, is 3a/2.

If A, B have opposite signs the form is au = sinh mO, (24) this has an **asymptote** parallel to 0=0, but the path near the origin has the same general form as in the case of (23).

This curve, bein~ an **asymptote** to its axis, is capable of being indefinitely proloi~ged towards X; but in designing pivots it should stop before the angle PTY becomes less than the angle of repose of the rubbing surfaces, otherwise the pivot will be liable to stick in its bearing.

To integrate this equation for a solid of given form is probably difficult, but it is easy to see that at some distance on either side of the body, where the liquid is sensibly at rest, the crest of the wave will approximate to an **asymptote** inclined to the path of the body at an angle whose sine is w/V, where w is the velocity of the wave and V is that of the body.