It is interesting to consider what the effect of such

185

conditions would be if they arose at the surface of our own

planet. We assume a horizontal force in the crust adequate to set

up tensile stresses of the order, say, of fifteen tons to the

square foot and these stresses to be repeated every few hours;

our world being also subject to the dynamic effects we recognise

in and beneath its crust.

It is easy to see that the areas over which the satellite exerted

its gravitational stresses must become the foci --foci of linear

form--of tectonic developments or crust movements. The relief of

stresses, from whatever cause arising, in and beneath the crust

must surely take place in these regions of disturbance and along

these linear areas. Here must become concentrated the folding

movements, which are under existing conditions brought into the

geosynclines, along with their attendant volcanic phenomena. In

the case of Mars such a concentration of tectonic events would

not, owing to the absence of extensive subaerial denudation and

great oceans, be complicated by the existence of such synclinal

accumulations as have controlled terrestrial surface development.

With the passage of time the linear features would probably

develop; the energetic substratum continually asserting its

influence along such lines of weakness. It is in the highest

degree probable that radioactivity plays no less a part in

Martian history than in terrestrial. The fact of radioactive

heating allows us to assume the thin surface crust and continued

sub-crustal energy throughout the entire period of the planet's

history.

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How far willl these effects resemble the double canals of Mars?

In this figure and in the calculations I have given you I have

supposed the satellite engaged in marking the planet's surface

with two lines separated by about the interval separating the

wider double canals of Mars--that is about 220 miles apart. What

the distance between the lines will be, as already stated, will

depend upon the height of the satellite above the surface when it

comes upon a part of the crust in a condition to be affected by

the stresses it sets up in it. If the satellite does its work at

a point lower down above the surface the canal produced will be

narrower. The stresses, too, will then be much greater. I must

also observe that once the crust has yielded to the pulling

stress, there is great probability that in future revolutions of

the satellite a central fracture will result. For then all the

pulling force adds itself to the lifting force and tends to crush

the crust inwards on the central line beneath the satellite. It

is thus quite possible that the passage of a satellite may give

rise to triple lines. There is reason to believe that the canals

on Mars are in some cases triple.

I have spoken all along of the satellite moving slowly over the

surface of Mars. I have done so as I cannot at all pronounce so

readily on what will happen when the satellite's velocity over

the surface of Mars is very great. To account for all the lines

mapped by Lowell some of them must have been produced by

satellities moving relatively to the surface of Mars at

velocities so great

187

as three miles a second or even rather more. The stresses set up

are, in such cases, very difficult to estimate. It has not yet

been done. Parallel lines of greatest stress or impulse ought to

be formed as in the other case.

I now ask your attention to another kind of evidence that the

lines are due in some way to the motion of satellites passing

over the surface of Mars.

I may put the fresh evidence to which I refer, in this way: In

Lowell's map (P1. XXII, p. 192), and in a less degree in

Schiaparelli's map (ante p. 166), we are given the course of the

lines as fragments of incomplete curves. Now these curves might

have been anything at all. We must take them as they are,

however, when we apply them as a test of the theory that the

motion of a satellite round Mars can strike such lines. If it can

be shown that satellites revolving round Mars might strike just

such curves then we assume this as an added confirmation of the

hypothesis.

We must begin by realising what sort of curves a satellite which

disturbs the surface of a planet would leave behind it after its

demise. You might think that the satellite revolving round and

round the planet must simply describe a circle upon the spherical

surface of the planet: a "great circle" as it is called; that is

the greatest circle which can be described upon a sphere. This

great circle can, however, only be struck, as you will see, when

the planet is not turning upon its axis: a condition not likely

to be realised.

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