CHAPTER IX

WATERS WITHIN THE EARTH

It has been estimated that approximately 1,500 cubic miles of water

fall upon the surface of the United States each year. About one-half

of this goes back into the atmosphere by evaporation; about one-third

of it flows away in surface streams; and the remaining one-sixth

enters the crust of the earth. Considerable water which enters the

earth returns to the surface as springs, by capillarity of soils and

rocks, or by being drawn up into plants and evaporated. Some idea of

the amount of ground water may be gleaned from the statement, based

upon a careful estimate, that all the water in the rocks and soils of

the first 100 feet below the surface of the United States would make a

layer seventeen feet thick. In most humid regions the soils and loose

rock formations are saturated with water at greater or less depths

(usually less than 100 feet) below the surface. The surface of this

saturated layer is called the ground-water level, or more familiarly

the "water table." The water table shifts up and down more or less

according to variation in rainfall.

In addition to the water held in the loose rocks and soils near the

earth's surface, large quantities occur in definite layers (usually

strata) of porous rocks which very commonly extend at various angles,

hundreds or even thousands of feet into the earth. A very fine

illustration of this principle is the case of the Dakota sandstone

formation of Nebraska. Almost anywhere across the State a well drilled

through a bed of clay and into the porous sandstone layer encounters

water. (Figure 19.) Another principle is also well illustrated,

namely, that water in such a porous layer may actually travel hundreds

of miles, water obtained from a well sunk to the Dakota sandstone

having actually traveled under the surface of the State all the way

from the eastern face of the Rocky Mountains, where rain and melting

snow entered the upturned and exposed porous rock layer. Another good

example is Iowa, where certain porous rock layers outcropping in the

northwestern and northeastern corners of that and adjacent States

gradually bend down under the State, reaching the greatest depths (up

to 3,000 feet) far in the interior. From wells 3,000 feet deep near

Boone, Iowa, it is, therefore, a fact that some of the water pumped

out of the earth actually traveled underground all the way from beyond

the corners of the State. This sort of travel of underground water is

common in many parts of the world. It should be clearly understood

that such water does not flow freely as in a pipe along subterranean

passageways, but rather it slowly works its way between the grains of

porous rock. Where such water moves distinctly downward, and the porous

layer has both above and below it an impervious rock layer like shale

or clay, it gradually gets under greater and greater pressure. In some

cases such pressure has actually been found by deep drilling to be

equivalent to that of a column of water several thousand feet high. The

rate of motion of water in porous underground rock layers is very slow,

data from various sources indicating a rate of speed of not more than

one-fifth of a mile a year in coarse porous sandstone, while in many

rocks it cannot be more than ten to fifty feet per year.

[Illustration: Fig. 19.--Vertical (structure) section from the Rocky

Mountains to Omaha, Nebraska, illustrating a widespread underground

porous rock layer (the Dakota sandstone) charged with water under

pressure, the clay formation acting as a cap rock. (After Darton, U. S.

Geological Survey.)]

We still have to consider a third mode of occurrence of waters within

the earth. Many formations, like granite and other types of crystalline

rocks are neither in definite layers, nor are they sufficiently porous

to allow water to really flow through them. Where such rocks extend

far down from or near the surface, how does rain water descend? It

does so along cracks or fractures (both joints and faults) which we

have learned are almost universally abundantly present in all hard

rocks in the upper (or zone of fracture) portion of the earth's crust.

Joint cracks are generally very irregular in direction and spacing,

while fault fractures are usually fairly regular and straight. Many

cracks are not wide enough to allow anything like good passageways for

water, while others are sufficiently open to allow water to travel

along them for hundreds, or even thousands of feet. In canyons of the

West, springs not rarely emerge from the bottoms of great, nearly

vertical ledges of granite and other hard crystalline rocks, the waters

certainly having entered the rocks hundreds, or even some thousands of

feet, higher. In rocks of the kind here considered it is evident, then,

that the movements of subterranean waters must be mostly exceedingly

irregular and usually not in great quantities. In many deep mines of

the world, underground water causes little or no trouble except often

near the surface. Occasionally a shaft or tunnel strikes a prominent

joint or fault fracture filled with water.

What we might really call underground streams may occur only under

exceptional conditions in rocks other than limestone, but in limestone

they are not uncommon because the slow solubility of the rock allows

underground waters to slowly enlarge the passageways to form distinct

channels. Echo River, which flows through Mammoth Cave, is a fine case

in point.

Most water by far which emerges as springs, was at one time surface

water. A simple, but common case is where rain water soaking through

porous soil (e.g., sand) or rock, sinks to the top of an underlying

impervious layer (e.g., clay) along whose surface it flows until it

reaches the side of a valley where a spring results. In fact, wherever

the water table is crossed by the surface of the ground, water must

either seep or flow out. Where underground streams which are common in

limestone regions reach the surface on hill or valley sides, springs

result. Another source of springs is where under proper conditions of

slope a porous rock layer, charged with water well below the surface,

appears at a lower level than its source of water. Still another type

of spring is where a fissure or fracture crosses a water-bearing layer

in which the pressure is great enough to cause the water to rise to the

surface along the relatively open fissure or fracture.

In various localities we hear of springs in seemingly paradoxical

situations on tops of hills and even mountains. Such a mystery is not

difficult to clear up. In the first place, such springs are rarely at

the summit of the hill or mountain. A case well known to many persons

is the small, but never-failing spring a little below the summit of

Mount Whiteface, a peak in the Adirondacks, rising 3,000 feet above the

general level of the immediately surrounding country. In this case, a

mass of highly fractured rock, subjected to much rainfall and lying

above the level of the spring, is sufficiently large easily to contain

and give forth enough water to account for several such springs. In

rare cases, however, springs or flowing wells are located on summits,

and in such places it is only necessary to bear in mind some of the

principles above set forth, but mainly the facts that water may travel

under pressure long distances underground, and that the point of

emergence may be on a hill which is actually lower than the source of

the water far away.

The economic significance of underground waters is forcibly brought

to our attention when we realize that 75 per cent of the people of

the United States depend upon wells for their water supply. Many city

supplies, most farm supplies, and much irrigation water come from

wells. The 3,000,000 people of Iowa, for example, are dependent upon

underground waters from wells varying in depth from a few feet to

several thousand feet.

[Illustration: Fig. 20.--Ideal section illustrating the chief requisite

conditions of artesian wells. A, a porous stratum; B and C, impervious

beds below and above A, acting as confining strata; F, the height of

the water level in the porous bed A, or, in other words, the height of

the reservoir or fountainhead; D and E, flowing wells springing from

the porous water-filled bed A. (After U. S. Geological Survey.)]

Most wells are simply dug to depths a little below the water table. In

humid climate regions the depths seldom exceed fifty feet. The water

encountered in such wells is rarely under pressure. In some regions of

deep soils or loose formations, wells are actually bored with an auger

to depths of as great as 200 feet. Deep wells in relatively hard rocks

are always drilled to depths of even thousands of feet. In such cases

the purpose is to strike either a porous rock layer charged with water,

or a crack or fissure filled with water, the water almost always being

under pressure (sometimes very great), under such conditions. These are

called artesian wells whether the water under pressure actually flows

out at the surface or not.

We may now inquire as to the necessary conditions for artesian wells.

This may best be done by the aid of diagrams. Figure 20 illustrates a

very common case where a porous layer, lying between impervious layers,

passing under a valley, comes to the surface of the hills on each side

where the water enters the porous layer. On sinking a well to the

water-charged layer, the water rushes through the hole to a greater or

less distance above the surface. In Figure 21 the porous and impervious

layers are simply tilted, and the water under pressure rises through

the free opening to the surface. Wells of this kind are also common

in the Atlantic Coastal Plain of the United States. In another case,

less comprehensible to the layman, the porous water-bearing stratum

curves downward under a hill or mountain, water entering it where it

is exposed on each side. Under such conditions a flowing artesian well

cannot be drilled at or near the summit, but since the water is under

pressure it will rise in the hole to a level approaching that of the

lowest part of the outcrop of the porous layer on either side of the

hill or mountain. This is essentially the condition of things toward

the interior of Iowa, where water from the deeper wells rises 2,000

feet or more in the holes, but does not reach the surface.

[Illustration: Fig. 21.--Section illustrating the thinning out of a

porous water-bearing bed. A, inclosed between impervious beds B and C,

thus furnishing the necessary conditions for an artesian fountain at D.

(After U. S. Geological Survey.)]

The drilling of deep wells, where records, including samples of rock

materials brought up, have been kept, has been a great aid to the

geologist in determining, or rendering more precise, the knowledge of

not only the kinds of rocks underground, but also the thicknesses and

structural relations of the formations.

In yet another way deep wells are of special significance, that is in

regard to the light which they throw upon the subterranean temperature

of the earth. Very recently the deepest well in the world was drilled

near Fairmont, West Virginia, to a depth of 7,579 feet, in quest of

oil or gas. At a depth of 7,500 feet, the temperature was found to be

168 degrees F. Allowing for a near-surface temperature 50 degrees,

this means an average rate of increase downward of 1 degree in 62

feet. The second deepest well is near Clarksburg, West Virginia, sunk

to a depth of 7,386 feet, with a temperature of 172 degrees at the

7,000-foot level, or at the rate Of 1 degree in 57 feet, allowing for

a near-surface temperature of 50 degrees. It is a remarkable fact,

that little or no water was encountered all the way down. A well 7,348

feet deep in southeastern Germany gave a temperature of 186 degrees

at the bottom, or a rate of increase of 1 degree in 54 feet. These

three records are about the average for the deep holes of the world.

Next to the deepest mining shafts in the world are in the copper

mining region of northern Michigan, where over 5,000 feet (counted

vertically, not down the slope) down the temperature is nearly 90

degrees the year round. The rate of increase is here less than in most

wells of such depth, because of the cooling air currents. Many years

ago a rather remarkable experiment in well drilling was tried by the

city of Budapest, Hungary, the attempt being to get a supply of water

at the brewing temperature of 176 degrees in order to encourage the

manufacture of beer. After getting a good supply of water at a depth

of 3,120 feet and a temperature of 158 degrees, work was stopped. In

building the two great tunnels (St. Gotthard and Simplon) through

portions of the Alps, such high temperatures were encountered that work

was continued only under great difficulties. In the famous Comstock

gold and silver mine of Nevada, over forty years ago, temperatures as

high as 157 degrees were encountered in the shafts at a depth of only

2,000 feet or a little over, the exceptional temperature for such depth

no doubt being due to occurrence of the ores in geologically recent

igneous rocks which have not yet cooled to the normal temperature for

the depth of 2,000 feet.

From the sanitary standpoint, wells are of very great significance,

especially in view of the fact that such a large proportion of people

depend upon well water. It is generally understood that typhoid

fever is more common in the country than in cities, in spite of what

might reasonably be expected. What are some of the causes leading

up to such a situation? The idea that water purifies itself after

flowing a relatively short distance is, in many cases, far from being

true, especially when we are dealing with underground water. Actual

observations prove that germ-laden water may travel surprisingly far

underground. Germ-laden water from barns, cesspools, or outhouses

spreads notably on sinking to the water table and it is easy to see

how so many wells become contaminated. On general principles, a

geologist is especially wary of water from a well in a barn yard.

The well for human use at least should be located out of reasonable

range of such contamination. Under the condition of the diagram a

well or spring some distance down the side of the hill may actually

be unfit for use, though a serious situation is much less likely to

develop there. Nor should one assume that by locating the well on

the uphill side of the house, and the outhouses or cesspool on the

downhill side, safety is assured. From what we have learned in regard

to earth movements, and the tilting of strata from their original

positions, we know how the movement of water in the saturated zone

near the surface may be downhill roughly following the hill slope,

while in a tilted porous layer of rock farther below the surface the

movement of water may be in just the opposite direction. A well drilled

into the solid rock for safety on the uphill side of a house might

derive its water from this very same porous layer, whose water has

been contaminated from a cesspool or other source down the side of

the hill. Such a case is by no means a theory or a rarity. There is

also real danger of contamination in cases where the water flows more

like streams underground through cracks or fissures in hard or dense

rocks, or through channels developed by solution in limestone. It may

happen that water becoming contaminated from barn sites, cesspools, or

outhouses finds its way along such a channel to the side or bottom of

a well. The author well remembers the case of a farmer whose house,

barn, and well were close together on a little limestone terrace and

who continued to use the well water although he complained of its

disagreeable taste, especially after a rain when he could "taste the

barn in it."

[Illustration: Fig. 22.--Diagram illustrating a danger of contamination

of wells by impure underground water. S, soil; B, bedrock; P, porous

stratum. Impure water from cesspool moves through porous layer to

bottom of well. (By the author.)]

Finally, in this connection, it may be said that wells should be

located in the light of the principles above explained, best of all

upon the advice of some one with geological training, and that, to

insure safety to health from the well water, sanitary analyses (at

small cost) should be made once or twice a year. A bad well should be

abandoned and a new one sunk.

A large amount of money has been wasted upon, and much mystery and

superstition has surrounded so-called "water witches," or those who

claim some special or supernatural power of locating supplies of

underground water. Most common of all devices used is the so-called

"divining rod," which is a forked stick of willow, witch-hazel, or

other wood, according to the seemingly special requirement of the

operator. Certain mechanical and electrical devices are also employed.

With one fork of the divining rod grasped in each hand and the main

part of the stick upright, the operator walks about until, due to

some "mysterious" influence, a place is found where underground

water pulls the upright portion of the stick downward in spite of

the grasp of the holder. Some operators even claim to know just how

deep a well must be sunk. Without any attempt to question the honesty

of all operators, geologists are in full accord with the following

quotation from a paper published by M. L. Fuller, for the United States

Geological Survey: "The uselessness of the divining rod is indicated

by the facts that it may be worked at will by the operator, that he

fails to detect strong water currents in tunnels and other channels

that afford no surface indications of water, and that his locations

in limestone regions where water flows in well-defined channels are

no more successful than those dependent upon mere guesses. In fact,

its operators are successful only in regions in which ground water

occurs in definite sheets in porous material, or in more or less

clayey deposits, such as pebbly clay or till. In such regions (which

are extremely common) few failures can occur, for wells can get water

almost anywhere. Ground water occurs under certain definite conditions,

and just as surface streams may be expected wherever there is a valley,

so ground water may be found where certain rocks and conditions exist.

No appliance, either mechanical or electrical, has yet been devised

that will detect water in places where plain common sense will not show

its presence just as well. The only advantage of employing a 'water

witch,' as the operator of the divining rod is sometimes called, is

that crudely skilled services are thus occasionally obtained, since

the men so employed, if endowed with any natural shrewdness, become,

through their experience in locating wells, better observers of the

occurrences and movements of ground water than the average person."

It should not be assumed, however, from the above statement that the

location or foretelling of underground water is mostly hopeless from

a scientific point of view. In most regions the kinds of rocks which

would be pierced by wells can be more or less accurately foretold by

careful studies of the rocks exposed at the surface. But foretelling

the underground water is often much more uncertain. Where the geologic

structure or arrangement of rocks in a region is fairly regular, as

in the case of most sedimentary rocks, and a few scattering deep

wells have been drilled, with records preserved, the geologist, by

combining such data with his surface studies, can do much toward

putting the facts regarding the underground waters of the region on a

scientific basis. There are many such regions, an excellent case in

point being Iowa, regarding which State the United States Geological

Survey has published a report containing data by the use of which

it is possible to foretell almost exactly what formations would be

pierced by drilling from 1,000 to 3,000 feet or more, the thickness

of each, which ones are water-bearing and, in many cases, even the

character of the mineralization of the water for almost any part of

the State. Such knowledge, through the years, is worth untold millions

of dollars to the State. Where the rocks are igneous and rather

uniformly dense, usually little or nothing can be accurately foretold

about the underground water supplies, because in such rocks the water

follows exceedingly variable and irregular cracks and fissures. In

metamorphic rocks the difficulties are usually about as great. In

limestone regions, with humid climate, much water travels in channels

underground, but these are so exceedingly irregular that there is no

way of locating them by surface studies. In humid climates it seldom

happens, however, that a well does not reach at least a fair supply of

water within a few thousand feet even in rock formations in which the

water travels along irregular cracks and channels.

Certain other important features of the geological work of underground

water should be brought to the attention of the reader. One of these

is its power to dissolve mineral substances of many kinds more or less

rapidly. As already pointed out, limestone is especially susceptible to

solution in water, both surface and underground.

The carbonate of lime taken into solution from limestone is the

principal substance which causes so-called "hard water." Most of the

solution takes place in the upper part of the zone of fracture of the

earth's crust and the dissolved substances are carried along generally

to the lower levels where they tend to deposit (and crystallize),

filling fissures, cracks, and even tiny spaces between mineral grains.

Cracks and fissures thus filled by mineral matter from solution

are called "veins." In many mining regions valuable ores and other

substances have been deposited from underground water solutions and

concentrated in veins. In many places underground waters with certain

substances in solution travel through various rocks or encounter

solutions of other substances and, as a result of chemical action, many

new mineral combinations result. Such actions through the millions

of years of geologic time have effected great changes in many rock

formations. In the case of petrification, like that of petrified wood,

the buried organism slowly decomposes cell by cell, and particle by

particle it is replaced by mineral matter from underground water

solutions. In this manner the remarkable so-called petrified forests

(not really forests) of Arizona and the Yellowstone Park were formed,

the petrifying material there having been the very common substance

called silica which is the same in composition as the familiar mineral

quartz. Mineral matter carried in solution in surface streams is

derived from ground waters which reach the surface. An idea of the

tremendous quantity of mineral matter thus removed may be gained from

the statement that by careful determination the Mississippi River

carries 120,000,000 tons in solution into the Gulf of Mexico each year.

[Illustration: Fig. 23.--Structure section and part of landscape in a

limestone region showing how caves and natural bridges are formed by

the dissolving action of underground water. AA, limestone; BB, sink

holes; DD, caves and galleries; and an arch (natural bridge) which is

the remnant of a large cave. (After Shaler, U. S. Geological Survey.)]

One interesting effect of the dissolving power of underground water

in limestone regions is the development of caves or caverns. Most

remarkable of all is Mammoth Cave, Kentucky, with its hundreds of

miles of passageways and galleries. This marvelous work of nature is

all a result of the action of underground water which has dissolved

and carried away vast quantities of limestone. Echo River, which flows

through the cavern, is still carrying on the work aided by various

underground tributaries. The stalactites and stalagmites, which are

so strikingly displayed in many caves, as at Luray, Virginia, in

which water with carbonate of lime drips or oozes from the roof and,

due mainly to evaporation, deposits the lime. Many wonderful and

fantastic effects are thus produced. Where part of the roof of a cave

is dissolved out, or falls in, a "sink hole" results. Where all but a

portion of the roof of a cave or underground channel has fallen in,

a natural bridge, like the famous one in Virginia, results, though

natural bridges are also formed by other means.

In concluding this chapter we shall briefly discuss hot underground

waters, hot springs, and geysers. There are two well-known ways by

which underground waters may become heated. One is by the movement of

water downward into the normally heated portion of the earth, the rate

of increase downward being, as above stated, 1 degree F. for about

50 to 60 feet. Water descending two miles would, therefore, attain a

temperature of about 200 degrees F. In some regions such a temperature

may be reached at depths considerably less. Such water (under pressure)

taking a short course to the surface (forming springs) at a lower

level would retain much of its heat taken up far below the surface.

In regions where there are great down-folds of the strata (i.e.,

synclines), as in the central to southern Appalachians, conditions

appear to be favorable for such warm or hot springs, as, for example,

at Hot Springs, Virginia. A second cause of the heating of underground

water is by the descent of surface waters into contact with masses of

still hot igneous rock of relatively recent geologic age. In some such

cases the water does not go more than some hundreds of feet down and

when, under proper conditions, it returns to the surface hot and even

boiling springs may result.

[Illustration: Plate 7.--An Upbend Fold (_anticline_) in the

Appalachian Mountain Strata Near Hancock, Maryland. The strata were

deposited in horizontal layers upon the sea bottom, covering the region

many millions of years ago in middle Paleozoic time. At the time of

the Appalachian Mountain revolution, near the end of Paleozoic time,

this and many other folds developed well below the surface. Removal

of overlying material by erosion has laid bare the fold as we see it

to-day. (_Photo by Russell, U. S. Geological Survey._)]

[Illustration: Plate 8.--(_a_) A Ledge of Igneous Rock (Granite) in

Northern New York. This illustrates so-called "joints" or natural

cracks, commonly separating most hard rock masses into more or less

prismatic blocks. (_Photo by the author._)]

[Illustration: Plate 8.--(_b_) A Fault Fracture in a Ledge at East

Canada Creek in the Mohawk Valley, New York. The Ordovician limestone

formation in thin layers on the right has sunk hundreds of feet along

vertical fault to the left of middle, bringing it sharply against the

older (Cambrian) massive formation on the left. The hole is artificial.

(_Photo by Darton, U. S. Geological Survey._)]

Geysers are periodically eruptive hot springs found only in a few of

the volcanic regions of the world. They are most wonderfully displayed

in the Yellowstone National Park, where they send columns of hot

water to all heights up to 250 feet at various intervals of time.

Almost incredible amounts of hot water are sent into the air every

day in the geyser basins of Yellowstone Park. The single geyser "Old

Faithful," which erupts at intervals of about seventy minutes, sends

a column of water several feet in diameter to heights of from 125 to

150 feet. During each eruption about 1,500,000 gallons of water are

sent forth, or every day enough to supply the need of a fairly large

city. A very brief explanation of the cause of geyser eruptions may

be stated as follows: The very irregular, narrow, geyser tube extends

nearly vertically downward into yet uncooled lava. The tube is more or

less rapidly filled by underground water. The bottom, or near-bottom,

portion of the water gradually becomes heated by the lava until finally

the boiling point is reached for that depth. But, because of the

pressure of the overlying water column, the boiling point at that depth

is considerably greater than for the surface. A little steam develops

far down and this causes the whole column of water above it to lift

slightly, thus relieving the pressure on the superheated water far

down. This relief of pressure allows much of the superheated water far

down to flash into steam, which violently forces the column of water

out of the geyser tube.

Geology: The Science of the Earth's Crust · 第 9 / 21 章