CHAPTER II

Imitating Ripplemarks

“_The Constitution is an experiment,

as all life is an experiment._”

At the end of the century my experiments with the sclerometer, and with

the class in experimental geology, steered me for years into laboratory

experiment. Europe was headed toward geophysics and geochemistry,

meaning chiefly mathematical and statistical analysis. My vision was

nonmathematical, though I used pressures, temperatures, clocks, and

yardsticks to measure erosion, sediment, warping of strata, and melting.

This took me away from petrography, for the polarizing microscope was

dealing with infinite series of minerals and molecules. I could see

nothing but infinite penetration into the smaller and smaller. Clarence

King and Frank Perret had been on the way to infinite journeying

outward to the bigger and bigger.

The guiding formula was “erosion, sedimentation, deformation, and

eruption.” Measure these on the globe, imitate them with mud pies

in the laboratory. Compare the global examples with the mud pies.

Try to get the mud pies to illuminate the gigantic stream systems,

flood plains, sea bottoms, folded mountains, intrusions, and lavas

of the earth. Then try to measure in the field those processes with

observatories. So, to me, came the transition from collections to

experiments.

The machinery of nature, whether with sand heaps or sand grains or

coral pebbles, is the same. It is impelled by currents flowing over

loose materials which make eddies in the lee of lumps. The eddies

are either billows or cyclones. At the middle they are billows; at

the ends they are cyclones. The billow eddies obstruct the heaping.

The cyclone eddies lengthen the heaps right and left of the current

direction. George Darwin studied the eddies by means of a drop of thick

ink in a glass tank on top of a ripple ridgelet. The ink migrated to

form underwater billows and cyclones, or vortexes. He used a dropper

to place the ink globule, and then watched the vortexes form as he

oscillated the tank.

Low parts travel fastest, namely the points. High parts build on the

upstream side, and travel slowest, and the stuff tumbles over the crest

line and is corniced by the eddy. Snow does it, pebbles under sea do

it, and marine life adapts itself to it, wherever the food supply is

best.

In the study of ripplemarks, Harry Gummeré, a graduate in astronomy,

was my collaborator. Ripplemarks are made by back-and-forth eddies on

the bottom, while big waves oscillate the water. We moved the bottom

instead of making waves in the water. A glass plate sprinkled with sand

under water in a tank was oscillated back and forth horizontally. It

was clamped under a carriage which oscillated on wire tracks stretched

across the tank. A string pulled the carriage against an elastic on

the other side. A wooden wheel and crank, set upright edgeways, had

holes and pegs to pull on the string, and the crank turns were timed

with a metronome. The holes in the flat wheel were a centimeter apart,

so that a revolution of the wheel pulled the string for every two

centimeters of travel of the carriage. Thus the sand-covered plate was

jerked back and forth under water two centimeters, four centimeters,

six centimeters, and so forth; once a second, or two seconds, or three

seconds, and so forth, by beats of the metronome.

The result was beautiful ripplemarks on a glass which could be lifted

out of the water, dried, and placed over blueprint paper to preserve

the record. The sizes of ridge to ridge ripples were from a fraction of

an inch to two or more inches. The little ones diminished to zero when

the jerking was small, the big ones washed out when the jerking was too

big.

The blueprints showed that both length and speed of strokes (amplitude

and acceleration of motion) made the ripples increase in size, and

somewhere between the largest and smallest sand ripples was the optimum

perfection of ripple form. The blueprints look like mackerel skies.

And mackerel-sky clouds are billows of condensation between an upper

cold stream of air and a lower moist one. In between are the same

back-and-forth billows of vortex as in our sand.

At a geological conference at Harvard I showed blueprints made directly

from glass plates covered with artificial ripplemarks. At the same time

I exhibited rock slabs of fossil ripplemarks and photographs of others

shaped like horseshoes. These were variants of the rippledrift process

seen on sandy beds of running streams. I also showed photographs of

swash marks running along the upper steep slopes of beaches. And of the

wind-formed rippledrift of dry sand dunes. From the deserts of Peru

come photographs of _medaños_, or crescent dunes, hills of sand

tapering to curved points at both ends. The points are downwind, the

high horseshoe toe of the hill is upwind, and like a coral atoll the

edifice is current-formed.

Ripplemarks can form in hundreds of fathoms of ocean water if the storm

waves on the surface of the sea are big enough. A particle of water on

the crest of a wave is lifted up and down in a long vertical ellipse.

A particle deep down under the wave is lifted fore and aft in a long

horizontal ellipse. Under a three-hundred-foot length of wave in the

English Channel in deep water the bottom particles of water are shoving

sand back and forth, and making packed ripplemarks.

A big sand grain becomes a lump for small sand grains to bump against.

They make a heap which piles up and lengthens out. The heaps merge and

we get a tightly packed and ridged sandy bottom. Each ridge has an eddy

first on one side, then on the other, as the water particles reverse in

direction. Oscillation builds first flocculence, then alignment, then

even spacing. The opposite sides of a ridge have equal slopes.

Rippledrift is made by a current in one direction. It is usually not so

regular or in such straight ridges as ripplemarks. If a stream of water

is jetted over sand round and round in a ringshaped tank, ridges will

migrate along the bottom, but they are smeary. The regular ripples in

dry sand on dunes have flatter slopes upwind, steep scarps downwind.

They are regular, probably because wind blowing is intermittent and

back currents occur. So they become more like ripplemarks.

On the bottoms of water streams, the horseshoe rippledrift requires

a nice adjustment of lumps and side points migrating downstream. All

rippling requires a sand of mixed sizes of grains. If they were all

alike they would not ripple, for the larger grains have to obstruct the

smaller ones in order to produce the ripple pattern. Rippledrifting

as a whole is a building mechanism. Mixed with wave currents which

move beaches along, including beach pebbles, it can be compounded

into building oceanic islands. The crescent dunes of the desert are

dependent on the prevailing winds being loaded with a sand supply at a

windward erosion source.

Oceanic currents depend on the winds, like the trades in the tropics,

and an obstructing bank or shoal adds surf action to the streaming. If

corallines and _Tridacna_ clams and crabs add organic cements, a

horseshoe hill is built on the sea bottom. Big eddies will do the same

kind of work as little eddies. This phenomenon extends all the way

from the galaxies of stars with their beautiful spirals, to the spiral

eddies in molten lava rushing down a pit crater, or to the streaming of

protoplasm in a plant.

De Candolle, the great botanist, studied rippledrift in order to try to

solve the most abstruse problem in all biology, the unsolved mystery of

cell division. At some critical point a budding cell decides to form

a partition and divide in two. Why or how? De Candolle thought that

the protoplasm granules circulating around the cell walls might start

regular lumps on those walls, and so build rippledrifts and make eddies.

Thus a current and an eddy and mathematics might start many of the

doubles, triples, hexagons, and stars of the world of shells and living

tissues. And the cells could pile up in symmetry in the submicroscopic

world.

The erosion of the earth’s surface reveals symmetries. River maps look

like trees with branches and with rivulets as twigs. Other symmetry is

in the horizontal plane of the ocean, where headland furnishes pebbles

and the sand sweeps into pure curves of beach and bar and cusp. So a

delta builds into a lake of leaf shape and annual layers are added as

the flood seasons come.

Some of the fingerlike drainage of erosion cuts into plowed lands

during a rainy spell. This suggests what might be done with a spray, a

mud bank, and a tank, to see how the finger valleys form. This erosion

of the runoff of water was imitated in the Harvard laboratory.

A beautiful river pattern on a slope, like the trickle of raindrops on

a windshield, was made by tipping up a rectangular glass plate covered

with very liquid clay. A portion clung to the glass, and exquisite

fernlike streams formed on the upper half of the plate, with a bank of

distributaries of V-shape on the lower slope.

This glass plate was used for a surface of stamp mill slimes, of

thicker beds, and was eroded with an atomizer and water by means of a

barbershop air compressor. The slimes are very fine pounded sands with

angular fragments. To get a stream pattern, this is necessary, so as

to have fine grit to cut down the rivulets between the coarse grit

remnants. This resembles the requirements for ripples.

The spray was kept going for hours. Meanwhile the river pattern at the

steep sides of the sloping plate ate into the bank of sediment, robbing

the streams of the main slope, because the side streams were oblique

cascades. They dug deep, took off the water, and left the main slope

streams without their headwater drainage. The pattern of the main slope

became the headwater branches of the side streams, the streams which in

plan drained over the edge of the uplifted plate right and left. This

was somewhat like stream robbery.

For example, the Lewis River at the south end of Yellowstone Park

once drained Yellowstone Lake, including the Lamar River, which is

now the headwaters of Yellowstone River. The Yellowstone plateau

formerly drained south into the Snake River and the Pacific Ocean.

The Yellowstone River headwaters suddenly tapped the system, thanks

to geyser erosion and acid corrosion, and the Yellowstone Canyon cut

down rapidly, reversing to the north the outlet of Yellowstone Lake.

Thereafter the lake flowed into the Mississippi and the Gulf of Mexico.

At some critical time about the glacial period the continental divide

made a leap of thirty miles from the present head of the Canyon to the

neighborhood of Lewis Lake, or from one end of Yellowstone Lake to the

other. This is stream robbery.

Spray and runoff and rainfall and wash did not alone cut down the

Yellowstone Canyon. The essentials were the rotting of rock and the

pull of gravitation on the fragments. The Yellowstone rotted away on

the north side, but it was hard granite and mountain-built quartzites

on the south, toward the Tetons. Hot spring rotting, geyser erosion,

acid waters, and sulfur decomposed the north country. The underground

water head followed the easiest channels, and the canyon was the

result. The canyon line encircles Mount Washburn, the old volcano, and

conceivably is over an old crack concentric to the dome.

Water is a transporter, and cracking opens ways to the rotting agents.

Only in rivulets and floods does water actually corrade, or grind, the

bottoms of streams. In our spray and fern patterns there is analogy to

rainfall springs on flat strata, but nine-tenths of the elements of

erosion are left out: jointing, weathering, ice, faulting, gravitation,

rotting down, quaking, solution, sliding, and last, spring water.

Erosion by sliding continues by wind action in desert mountains, and

on volcanic cones under bombardment, and by rocks snapping under chill

and sunshine on the moon. Creep of loose stuff is the greatest eroder

on earth. Rainfall cloudbursts certainly help, especially where soil is

not held together by a mat of roots.

The process of erosion is supposedly slow, as all geological processes

are slow, if we neglect the possibility of such submarine landslips

or supramarine upheavals as occurred at Yakutat in 1899. But even

New England has floods, hurricanes, landslides, forest fires, and

cloudbursts which are exclamation points on an otherwise sleepy

history. And in the past it has had ice sheets, and subsidences beneath

the sea.

In other words, the making of valleys and stream patterns for the

map is accented occasionally, and the occasions may come in climatal

waves unknown to us. The stream patterns in the Bad Lands, Tennessee,

Pennsylvania, the Grand Canyon, and New England make very different

maps. The rotting of the rock, limestone caverns, rainfall, faults, and

sloping underground strata bearing spring water all influence these

maps. What is erosion and what index is written on the land to say the

Grand Canyon and tributaries are being carved downward faster than the

Mystic River in Boston?

Ralph Stone tackled the Mystic River, and marked ledges and set stakes

opposite the flood plain meanders. The idea was that ledges split by

winter freezes, and that the meanders of a stream build on one side

and cut on the other. Maps were made repeatedly, and the ledge cracks

were measured in millimeters. Some movement was found, but a college

year was not enough time. If we could combine as a motion picture,

photographs from the air taken once a year for many years, doubtless

the film would show that the stream meander pattern is migrating toward

the sea like a wiggling snake.

Stone next made a model three inches thick in a tank of water, by

sedimenting sixty-one very thin layers of marble dust, coal dust,

clay, red lead, and sand. He tipped it up as an island and sprayed it

in periods which lasted one to ninety-two hours, up to a total of 719

hours. A forking stream and its delta were formed in the lagoon of

the tank. The stream cut a canyon with waterfalls, treelike branches,

esplanades, and a flood plain. There were three principal hard white

multiple strata layers in the model, separated by sand. The white

layers made waterfalls and were eaten back to form the canyons.

When the cross section of the delta was sliced with a knife, it showed

three white layers foreset at thirty degrees under the tank pool

and separated by more sandy strata. The bottommost of these was the

sediment of the top thick marble dust layer of the model as first

eroded by the spray, and the top frontal layer of the leaf-shaped delta

was the product of the erosion of the canyon bottom on the lowest of

the white layers. This must happen in nature where one formation in

reverse order is derived by river erosion undermining a stratified

older pile of sediments.

We called this the Grand Canyon model, and it showed many features

similar to those of South Dakota Bad Lands and the Colorado River

drainage. It was strictly rainfall erosion and stratification soakage

and seepage. The model surface sloped ten degrees, the high divide

at the top had a backslope of forty-five degrees, and everything was

sprayed for two months with special hose nozzles, making during part of

each day a mistlike rainfall.

The steep backslope did not trench itself at all despite its steepness.

This slope, on the contrary, absorbed moisture and carried the rainfall

underground down the dip of the strata to add spring water to the main

streams. The backslope was a “steep escarpment,” supposed in physical

geography to migrate by trenching backward, but the rills never gained

volume enough to cut into it. All the water volume acquired its grit

for cutting from the large surfaces, which were gradually tilted in the

direction of the rivers.

When the complete series of experiments on erosion and sediment

was published, it showed that the treelike branching of rivers is

dependent on underground water surfaces; that meanders on a flood plain

are partly a bubbling-up process of flood-plain soakage; that when

side tributaries form by undermining, the upstream branches cut off

underground water from the downstream branches; and that when a country

is tilted in one direction, there is a tendency to parallel streams,

separated by intervals controlled by underground water areas reached by

the undermining tracery of headwater springs.

This arborescence in a spray model is a regular and delicate

adjustment, where a bunch of tributaries is not mere catchment of

rainfall, but is the product of sheet flood in belts of underground

water related to the tilt of the country. Arborescence of river

drainage on a surface of flat strata, like the coastal plain of the

southeastern United States, is a rhythmical pattern of exquisite

design capable of reproduction and study in the laboratory. It is a

mathematical forking and headward development dependent on volume

of water, undermining impermeable strata along permeable ones. And

after the “tree” map is formed, the bulb of branches and twigs and

underground leaves of spring water holds all the downslope country in

its “shadow,” so that no new rivers can form there. This is what makes

our great maps of river systems. It is not haphazard. It is a vast

ocean of underground water, with mountains of water and valleys of

water.

A great lake marks an underground soakage water level. A riverbed marks

an underground seepage topography. The sea of water inside a continent

is just as much a map of hills and dales of water as the land is a

map of the hills and valleys of geography. The water is dynamic, it

is flowing. The land surface is dynamic and rain fed; it is creeping

soils. Together, groundwater and rivers are melting down the landscape

as a living thing. Man dams the water and uses the power of the erosion

melting down the land.

When we went to Haystack Basin north of the Yellowstone Park, we found

that all of the mountains surrounding it were audibly crumbling.

Ultimately, the continent is all one thing: a falling body of rotten

rock, ice, water, sand, boulders, and soils, self carved into valleys

and mountains, always tumbling. And down below are the fault blocks,

prisms of earth shell over the white hot core. And that also is

eternally in motion, irrupting, earthquaking, lifting, falling,

scraping, heating, cooling in waves through the ages. Man is very tiny,

but if he listens he can hear the earth’s heartbeats.

At hot springs the water mantle meets the hot earth shell. So the

geyser basins of Yellowstone, California, New Zealand, and Iceland are

a hot part of the great erosion system of groundwater. This brings us

to the next group of experiments, the making of artificial geysers.

Geysers as eroders show that the under earth is hot and is invaded by

rainwater. In exceptional volcanic places the water is boiling hot. The

Firehole River of the Yellowstone is carving down basins of solution

faster than the regular geysers are building up siliceous sinter. Here

is boiling-spring erosion by solution. It may be called the extreme

thermal aspect of ordinary spring-water erosion. How does spring water

erode? By bubbling up under the beds of rivers. The bubbling out of

springs starts rivers, and flood rainfall starts soil gullies; land

sculpture is the result.

We introduce geyser experiments here because boiling springs make drama

out of ordinary springs, just as active volcanoes make drama out of

buried volcanoes. Ordinary springs and buried lavas intruding invisibly

are much more important and extensive than geysers and volcanoes. Most

people never think of a spring as one of millions bubbling up the beds

of brooks and rivers and sea bottoms.

Most people never think of volcanoes erupting--properly speaking,

irrupting or inrupting--under Kansas or Brazil. Nobody denies those

places are hot underground, but it all seems remote. Yet every spring

is thermal if there is heat escaping through the rocks around it.

Geyser basins lower the country around them and leave hills in relief.

The proportions of basins and hills depend upon the runoff of rotting

and dissolving rock. The shape of a hill standing high, what Davis

called a monadnock in New England, depends on its whole history, not

on its hardness. Ascutney Mountain stands high as a lump because

surrounding slates have rotted down. Mount Monadnock may stand high

because the springs under the river pattern of cracks neglected it in

the rotting and crunching of a continent.

Dynamic weight eternally falling makes low places. Hardness against

weathering makes a mountain high only as a relic or residual. It is

a node in the gigantic process of gravitation rotting and the spring

squirting of groundwater. The water heats, rises, dissolves, siphons,

springs up, and transports dirt. Underneath is a definitely heated

earth crust.

Accordance of summit levels of mountains and hills as one looks across

country does not have to represent an upraised plane surface. There

is more undermining where the spring squirting is most voluminous.

When spring squirting is equal, the opposed slopes of a valley adjust

themselves. The tree line, the snow line, the rain line, and the wind

line are definite levels of erosion. Under it all the rotting rock is

falling toward the earth’s center, slowly, creakingly. The everlasting

hills are not everlasting, they are everfalling; rocks, boulders,

slopes, waters, gravels, sands, and muds. And adjustment to the

atmosphere and groundwater surface is irresistible.

[Illustration: _1. Experimental Geology Laboratory, Harvard

University, 1900_]

[Illustration: _2. Fountain at edge of lava lake, May 17,

1917_]

The notion of erosion pulling down hills to a flat plane near sea level

is fascinating to geometry-minded people, but not to the mechanically

minded. A flat plane near sea level in the Mississippi delta is

where the river has swung right and left against valley walls, over

its own flood plain. A flat plain, secured by ice sheets or planed off

by encroaching wave action as land sinks is mechanically probable. In

these circumstances we look for river or ice or wave-beach deposits.

But an “almost plane” occasioned by the multiple action called erosion

down to base level is to me the delightful dream of map students. If

a landscape has been planed off, a machine router or planer did it.

The great rivers of China have had a long time to bang back and forth

against their confining boxes of rock and on top of their own mud.

To return to geyser-spring experiments, I built a simple quart flask

surmounted by a four-foot glass tube. At the top the tube rose through

a cork in the bottom of a two-foot pan. In the side of the cork of the

flask was a second tube with a hose leading up to a reservoir bottle of

water. The reservoir bottle could be raised or lowered. If the water in

it was level with the pan, there was hydrostatic equilibrium: the pan

a pool, the bottle a source, the flask and tube full. When we applied

heat to the bottom of the flask, the water boiled, the pan overflowed,

and some cold water from the bottle chilled the flask. The pan had

become a boiling spring.

Next we lowered the reservoir bottle. The reduced head of water

permitted no overflow at the pan, and steam bubbles accumulated in the

four-foot upright tube. The boiling point was controlled by four feet

of water pressure. If the bubble lift reduced this to three feet, there

was a lower boiling point, the pressure was reduced by overflow above,

and the whole flaskful boiled. The geyser tube became a regular geyser

at intervals of a minute and a half, with eruptions enduring twenty

seconds.

This was a miniature of Old Faithful in the Yellowstone. Old Faithful

is bigger, its intervals average sixty-five minutes, and they range

from thirty-one to eighty-one minutes. It jets up 150 feet for a period

of four minutes. It throws out 3,000 barrels of water at each eruption.

Our little machine threw up about a pint to a height of four feet.

We hear much about soaping geysers as an artificial stimulus. The

apparatus in our laboratory showed the effect of soap right away. When

some soap was put in the pan, the intervals of a minute and a half

shortened to one minute. Soapsuds accumulated in the tube and depressed

the water to the neck of the flask. The multiple bubbles, film against

film, made the water system viscous. The myriads of tiny steam bubbles

formed so fast that they shortened the lifting time for the column.

If the height of the reservoir bottle was so adjusted that the geyser

didn’t quite know whether it was a geyser or a boiling spring, the soap

made the decision, and the thing went off with a bang.

This simple group of experiments makes springs very real. The

Yellowstone explosive springs differ from other springs in having

superheated steam from live lavas to heat them. The rock is cracked and

the water is doing a job of solution and deposition. It deposits stout

tough silica around some openings and builds them up against the head

of groundwater, and they become geysers. It deposits lime dissolved off

underlying limestone at Mammoth, and this makes sculptured terraces

but not explosive springs because the temperatures are not so hot. In

both lime and silica regions, blue-green algae, which love hot water,

decoratively sculpture the pools.

Like a magician I exhibited the artificial geysers before New York

and Boston science academies, and gave the summaries of the results

of our geyser experiments, as follows: (1) Boiling springs are like

other springs, controlled by the head or pressure of underground water

in the hills. (2) Upstreaming of heated water and building up of

silica (convection is the scientific jargon) may push the vent of a

boiling spring even higher than its source (reversed head). (3) In this

delicate condition, even rainfall or sinter building up or outburst

at a lower level or clogging of a pipe may change spring to geyser or

geyser to spring. There are many more boiling springs than there are

geysers, and many more hot springs than there are boiling springs, and

the word cold means nothing at all. There may be boiling springs under

New York City if you go deep enough. That is why the riot of geyser

apparatus is worth thinking about. (4) Irregular geysers overflow

continually, regular geysers discharge their waters only during

eruptions. Both are methods of feeding rivers, just like any other

springs. But there is a lot of volcanic heat underground.

This brings up the question of how much a volcanic eruption is like

a geyser. Geologists apply a glib word, phreatic, to Japan’s Bandai

Volcano, which blew steam and rocks out of the side of a mountain and

dammed a river. Hawaiian volcanoes squirt liquid basalt up a crack

with flames and red fume and sulfur gas, and almost no steam at all.

The answer seems to be that the Palisades of the Hudson may once have

been Hawaiian lava eruptions and, further, that lava is still erupting

there if you go down deep enough. New York doesn’t know about it, but

it sensed it in 1886, when it felt the Charleston earthquake.

All that Catskill water supply of the great city is in cracks above the

level of the deep lava, and extends out under Long Island Sound. If the

Hudson fault fissure wiggled a little more than usual, and if the deep

lava lowered and pulled down some of the Atlantic water, an eruption

like Bandai is not impossible in the Watchung Ridge of New Jersey.

This is not likely; but the globe has been through revolutions and

cataclysms, and the Watchung explosions might start a new geyser basin.

Something like that happened in northwest Wyoming in the Pliocene

age, during 11 million years, next preceding the ice ages that began

2 million years ago. And the Yellowstone was the result. We shall see

more volcano geysers.

Next, the making of deltas became a hobby in our laboratory, in

connection with the old leaf deltas scattered on the New England

landscape, partly covered with trees within the grounds of the country

villas about Boston.

Delta deposits extend upstream, within the mould of the cavern within

ice of the glacial period. Thus the map shows a snake-like ridge of

gravel, ending in a maple-leaf flat, with lobate frontal slopes. These

slopes were much steeper where the dump of the stream on the delta fell

over the beach line at the lagoon or lake level in which the delta was

built. This was like the delta shown in Stone’s erosion model.

Stone prospected the idea of torrential deltas in a tank, while E. W.

Dorsey and I started a tank imitation of the glacial sand delta. In the

glacier, the ice tunnel had been supplied with water by melting through

the ice crevasses, just like tunnels seen in Switzerland, floored with

sand ground up by the ice. There was thus a torrent pouring along

inside an arched tunnel, the mouth of which emerged on a delta in a

pool, with water surface either at the tunnel level or above it against

the rounded front of the ice mass.

In imitation of a rounded bank of ice with a pool of water in front

and with a subglacial meandering cave fed with sands and a torrent,

an apparatus was built and supplied by a hose. A sheet of lead was

bent in the form of the glacier surface, with an arched opening, and

set in our tank. This fitted over a tunnel of sheet iron, soldered

so as to meander in plan, and fitted at its upper end with pipe and

hose connection. A sheet-iron funnel rose from the upper end of this

artificial cavern, wherewith to supply different colored sands to the

model subglacial river, represented by the hose jet and iron tunnel.

The iron tunnel ended flush with the leaden arch.

The object of the experiments was, first, to set the leaden glacier

in a pool of water in the laboratory tank. Next, to jet water through

the tunnel, supply sediment in successive colors through the funnel,

and let that accumulate on the bottom of the tunnel and in a delta

in front of the artificial leaden glacier. The deltas and their

sliced cross sections in different experiments represented the noted

difference of kinds of sand supply or difference in water level of the

pool. In one case the water level was below the ceiling of the tunnel

where it emerged from the arch entrance. In another, it was above the

cavern mouth, so that water of the cavern stream, debouching from the

submerged cavern mouth in the lagoon, spurted up with its mud and made

a half crater against the glacier front.

These experiments illuminate the gravel-quarry sections of

Massachusetts. In those cuts in eskers (serpent ridges) and sand plains

(glacial delta fans) were seen topset beds, or flood wash, or foreset

beds at forty-five degrees which are the sublagoon frontal wash, and

occasionally backset beds where cavern wash gushed upward.

So our cross sections, cut with a knife in the delta, and the winding

cake extending upstream in the cavern showed topset, foreset, and

backset strata after draining the tank and lifting out the apparatus.

From the embryo delta the flood-plain beds overlap the earlier frontal,

or foreset, beds. The frontal beds are always under the lagoon. The

flood-plain beds (topset) were made by a meandering river course under

the air. Always this plain is built at beach level as a wash fan shaped

like a leaf, with the cavern stream bottom as the stem of the leaf.

New England has been covered with mountainous ice, miles high.

Subglacial streams and subglacial clear ice caverns are abundantly

found at the lower ends of all glaciers in the world. They merely

represent the melting snow and ice in pulses of sunshine, snow at the

source, ice in the course, crevasses and gravitation making water seep

through. This water shapes a channel for itself and erodes a sewer

system of scouring along the bottom of the subglacial valley. This

grinds and melts the bottom ice into arched caverns; and the sediment

builds up on the stream bottoms, eventually carving the roofs of the

caverns into high arches or arcades. The subglacial caverns are self

constructed drainage pipes.

The glacial stream is really a river flood cutting its valley. The ice

river grinds and scrapes, and the water under the ice pipes and drains

the melting. The ice carries chisels of broken rock. The enormous

weight, in gliding plane layers of ice, flows in accordance with the

crystal laws of snowflakes and ice crystals. The moraines, or debris

fields, at the sides and on top and underneath the eroding ice jumble

yield mud and sand and boulders. The torrent underneath removes the

rubbish.

The delta in front follows laws of sedimentation. If there is no lake

in front, the delta is a flat wash fan, or valley flood plain. All

these things become clear to the student who makes a baby glacier out

of tinware, sand, a tank, a hose, and a faucet.

I have spoken of cataclysms, or what early geologists called

catastrophe, happening occasionally in the world of erosion and

subterranean geysers. Such were the Yakutat crash and the Bandaisan

explosion. But each glacier-period field, like an ice mountain over

Europe and America, constituted a cataclysm lasting 500,000 years,

and this happened four times even in the centuries of early man. The

Mediterranean and the Great Lakes are offspring of such cataclysms.

But Lyell carried the doctrine of uniformity to extremes; he thought

that what man sees is what always happens. I do not believe Lyell ever

realized that earth or sun might conceivably explode in a month of our

time. Again, this is not likely.

The opposite of uniformitarianism is occasional catastrophic trigger.

The process of erosion pulls the trigger for sudden deformation. Slow

deformation pulls a trigger for eruption. Eruption triggers internal

intrusions. The Frank Landslip; the Charleston, San Francisco, and

Napier earthquakes; the Pelée eruption; and the Yakutat upheaval all

created terrific surprises for geologists.

The gigantic intrusions through millions of years from the core of the

earth, made of white hot star matter, percolating to surface volcano

belts up 1,800 miles of permanent, primitive cracks, are mostly

balanced by the crustal weight. This is the adjusting globe. But the

intrusive mechanism, under tides in the rock and in the oceans, always

in motion, pulls the trigger for the big geologic revolutions.

The very deep broken earth blocks shift, volcanism between them heats

the surface, floods the surface with gas foam, and lifts areas of

surface by heat swellings; and on the surface, what was a glacial

period gives place to a volcanic period. The last of these was the

Miocene Tertiary, with large-scale volcanic eruptions all over the

world.

Comparing Boston with the Black Hills showed underground eruptions in

the latter, for which a warping uplift pulled the trigger. These were

the rock cisterns or lenses of porphyry injected among the strata. The

time of this was Miocene or Eocene Tertiary, probably later than most

of the volcanoes of the Yellowstone, farther west.

Boston, on the other hand, was making black basaltic dikes, probably

identical with the volcanoes of the Berkshire Hills and New Haven, of

the age of the big reptiles, 150 million years before the Black Hills

injections. The trigger which pulled off the Boston eruptions was the

Appalachian warping. That which fired off the Black Hills was the

Laramie revolution that pushed up the Rocky Mountains.

The injection of lava lenses in the Black Hills was a form of

deformation of strata which we experimented with in the laboratory. The

layers of sandstone, limestone, and old ocean muds covering over the

arch of these hills were injected by dikes or fissure fillings from

below. How would injections behave?

With Ernest Howe as my associate, I arranged a square tank for

sedimenting sand, plaster powder, coal dust, or marble dust in layers

under water. Under it was an iron cylinder in which wax could be

melted. A screw piston pushed the molten wax up to inclined or upright

slots in the middle of the tank box. The water was drained off, and

the hot wax was injected up into the strata. The tank sides were taken

down, and hardened lenses of wax were sliced vertically with a hot

knife to show what had happened to the strata by the process of wax

intrusion.

In some of the experiments 300 pounds of shot were piled over a cloth

layer on top of the strata to imitate the weight of natural sediments.

This was before injection of the hot wax, and the result was a neat

dome of deformed layers at the surface, a domical hill over a lens of

wax inside. This hill was eroded with a spray of water to show what

kind of radial valleys would form. Such radial streams were found in

South Dakota, with infacing escarpments, around some of the dome hills

made by laccoliths.

From the beginning it appeared that a lens of injection would form,

that the strata would arch over a dome of wax. The arched strata

stretched on the crest and the breaks gaped upward, while the side

bends cracked gaping downward. It was there that the wax could break

its way upward and make a volcano. Some nice little experimental

volcanoes of wax-built cones and craters formed on top of the model.

As with all folded strata arched downward under weight, the cracks

on the bend of a downward arch, or syncline, admit lava from below,

whereas the cracks on the upward arch, or anticline, are held tight,

closed by the weight of strata above. Thus an intrusive dome will not

erupt through its crest, but through its sides.

The results of all these tests showed that rigid beds carried the

arching force and that soft beds were most invaded and pushed aside by

the wax. The steepness of curvature of arch varied with the load. An

inclined pipe formed an irregular lens thickest away from the incline.

In a hard bed ruptured on a downbend, concentric fractures around a

dome let the lava up to higher strata.

On the crest of a hard bed the fractures are like the spokes of a

wheel, but they do not make dikes; they yawn open upward. Liquid wax

tended to spread as a thin sheet in soft layers of strata, stiffer wax

tended to arch up in a steeper dome. Rapid injection made a higher and

smaller dome than slow injection.

Compared with the arching up the whole long mountain oval of the entire

Black Hills dome, with granite on the crest, this intrusion of wax

only imitates the small domes of lava intrusion or injection, where

the injection carries the energy or stress. Indeed, in nature, even

the lava lenses are influenced by the buckling that is going on in the

strata under stresses of crust warping. For the warping crust of the

earth is always pulling the trigger and straining the strata. The lava

rising from below seeks out the weak places and assists the buckling,

as well as following the most incoherent mud or shale beds.

When it comes to the big oval of the whole Black Hills uplift--swollen

up like the Rocky Mountains during millions of years and within which

the lava injections were only an item--we are dealing with a push from

below or an expansion that swelled up the pre-Cambrian ancient rocks as

well as the later granites. Such swellings were doubtless made again

and again in Massachusetts. There, also, we find lavas and granites and

Red Beds and glacial boulders, older than the Appalachian Mountains,

as well as younger. The younger Triassic lavas are definitely erupted

between fault blocks.

All that our experiments showed was what melted stuff will do in

strata under weight, when the force of melted stuff overcomes that

pressure to find a place for itself, although the weight may be more

or less lifted by big arching that is taking place on a big scale. The

arching is bigger than the hydraulic or gas pressure squirting.

There is another possibility besides buckling. This is faulting, or

movement of deep crust blocks the boundaries of which do not appear.

The deep crust is a movable mosaic above the core, and this movement

renews itself, now here, now there. Dutton shows that we may think of

the Rocky Mountains this way all the way out to the Pacific coast. We

may have the core fluids sucking down the blocks, the volcanic fluids

pushing up the local strata. And the volcanic fluids in cracks are the

degenerate gassy top remnants of the core fluids which man has never

seen and which are 1,800 miles down.

The boundaries of the crust blocks do not appear because the whole

first shell of the globe is buried under lavas and intrusions and

crystals and mud, meaning by mud, countless dumpings of lakes and

rivers and seas through 3,000 million years. Such is the kind of

thinking started by making wax injections.

It will be seen from the experiments that whether we are imitating

underground heat with a Bunsen burner to start a geyser, or overground

cold with delta apparatus to simulate a glacier, we are dealing with

erosion of the earth’s surface. Erosion started with the first attack

on lava by the atmosphere or by sea water. Never was the pristine

lava anything like the magma inside the globe; it snapped and chilled

and oxidized. Whether we call it basalt or obsidian, it degenerated.

Moreover, it degenerated in the outer crust when it loosed its gases,

heated itself and the rock wall, found groundwater and free air, and

started oxidation new to it. Thermal action is just as much concerned

with erosion as is rainfall or snow. Therefore, whether injecting

wax and swelling strata or imitating geysers and ripplemarks, we

were experimenting with volcanoes, for the crust of the earth is

fundamentally volcanic. For the purposes of this book these facts

demand reiteration.

In what are called geosynclines, or earth sags, the great beds of

strata are accumulated. They are the dirt washed from highlands into

midland seas. They are strata of sandstone, mudstone, or limestone;

thin films in comparison with the fire-made earth crust. It was

the wrinkling of basin fills by expansion or end push that built

Himalaya and Appalachia. The mountains are etched out of foldings and

overthrusts and faults by rotting and water transport. Pressing the

strata endways to wrinkle them is called mountain building, much better

named strata wrinkling. The thickest of them reached twelve miles

vertically, but what is that to the earth’s crust of 1,800 miles? The

crust lifts and lowers fault blocks. The little strata basins expand

with heat on their bottoms and get pulled and pushed by underground

lava intrusions. Also they get squeezed by global contraction between

crust blocks, and shoved up and down by the agelong wobbles. The

biggest wobble was the downdrop of the great oceans over fault blocks

when the crust first cracked and settled over the core. Those oceans

have shifted and adjusted in waves of global action ever since. The

crust has kept the earth a sphere while lavas erupted and weighted down

the blocks. This block wobble extends into the innermost continents.

Eruptions up the cracks migrated from the continental seas to the

shores of the present oceans. They changed composition as they did so,

because they changed from under-air eruptions to under-sea eruptions,

fifteen pounds pressure to 600 atmospheres pressure. From erosion

eruptions with enormous heat, to deep sea eruptions with enormous

chilling and pressure. And the latter are the volcanoes of the present

day, mostly concealed except for the islands and sea borders.

Meantime, the crust blocks continue to wobble up and down, and quakes

continue to creak under the rock tides of sun and moon pulls. The

creaks and wobbles are our big earthquakes, tidal waves, and eruptions.

Such big accumulations of eruptions as the Cordillera or the Hawaiian

Ridge is a terrific weight in a few million years. Both heaps have been

at it since Miocene time, or for about 18 million years, banging down

through the crust blocks on top of the core. Whether such balancing

of heavy weights on top of the crust blocks is due to change of lava

weights or sediment basins, six to twelve miles of rock vertically, the

down squeeze and underflow is called by the Greek word isostasy. It

means standing level and is a poor word because the earth’s crust never

stands still. The blocks are eternally adjusting and creaking over a

fluid core, the globe is whirling, the sun and moon are pulling, the

volcanoes are erupting, and the solar system is shooting through space.

Terra firma is never static. And our little atmospheric lives on top of

it never stand still. We are hot, and we ourselves do a great deal of

eroding.

This oration is introduction to the next series of Harvard experiments,

which dealt with squeezing and wrinkling strata in imitation of the

folds and faults of the Appalachian Mountains. Bailey Willis, at the

Geological Survey, made a press of wax models of strata. A heavy oak

piston was advanced by a screw crank. The models were waxes mixed with

plaster for hard strata and waxes mixed with Venice turpentine for soft

strata. They were cast to imitate actual successions of hard, thick

limestones; less hard sandstones; soft mudstones; or slates. The piston

advanced at a measured rate against one end of the model, the other

end being a fixed box, the strata lying horizontally. The elongate

Appalachian basin had a continent (the piston) to the east; a wide flat

fill of limestones or sea bottom to the west (the box); and the deepest

trough of pebbles, sands, and muds on the east, toward the rivers of

the eroding continent of that ancient time. The heavy limestone tapered

from the west into these thinner beds and made a stiff rib in their

midst. The final result of their wrinkling was linear folds with axes

north and south parallel to the trough, and close set at the east.

The folds overturned toward the west, the overturns developing into

overthrust fractures westward when the beds ruptured. Also, the folds

became bigger, flatter, and wider apart westward under the deeper sea,

the famous one being the Cincinnati arch.

The evidence in the middle eastern states is that the trough bottom

sank as the heavy shore sediments were dumped by rivers into the sea.

The west-central states received a wide flat of limestone. Uplift of

the continent shallowed the ocean and pushed it, narrower, over to the

great plains. So there were left a deep trough of weak beds, a massive

limestone, and an overlap of continental wash across the uplifted later

continent of the present time. The problems to be studied in Willis’

models were how folding would affect such a pile, what transmitted the

wrinkling force, what started a single fold, and how soft and hard

strata behaved under horizontal pressure.

He found that hard, thick layers of limestone transmitted the push

farthest. That soft beds piled up on each other near the piston. That

these beds showed beautiful overthrust faults inclined away from the

piston. And that the start of individual folds was favored by very

small initial bends in a transmitting layer. These downbends away from

the continent would be made as the trough bottom sank through the ages.

The nature of this sinking in upright slices of the bottom rock is

probably downfaulting. Each vertical slice would make a step-bend as it

sank.

The bottom of Willis’ box did not admit of down motion by underflow,

nor did the piston pressure create an opposed horizontal force that

might have come from the ocean area. In restraining up motion over the

folds that formed, Willis piled bags of shot on top of the model to

represent downweighting. The folding in the Appalachians was down at

the bottom of the heap where things were hot and compressed, and heat

could extend individual strata.

In our pressure chest we extended the Willis conception. We made two

pistons at opposite ends of an oaken box, with thick plate glass

panes at one side, so as to watch the folding. The two pistons would

distribute the end pressure better and admit the possibility that all

the pressure did not come from the continent. The bottom under the

model was an inner box that could move down, hung on heavy spring

balances. These could be screwed up to a pressure upward to compensate

the load of shot. Thus the first fold could arch downward as well as

upward. This imitated a possible lowered trough bottom. The piston rate

of advance was controlled by metronome, one man at each screw.

For examples, models E, F, and G had four white and four black layers,

all alike in substance, at fast, medium, and slow rates. The quickest

was shortened one inch in five minutes. The slowest was one inch in

an hour and three-quarters. The quick-squeeze model flexed smoothly,

all folds seemed to flow, and the model held together compactly. The

slow-squeeze model shortened the same amount, cracked in many places,

was brittle, and did not hold together compactly. This appeared to

prove that slow motion will fracture where quicker motion will hold

strata intact, under otherwise identical conditions of substance, of

folding and shortening, and of vertical confinement.

We verified Willis’ conclusions that stiff and thick beds transmit the

pressure farthest and that overthrust tends to form in soft beds, which

thicken near a piston. In one model we got overthrusts in opposite

directions on opposite sides of the model along a single-fold axis,

with a twist in between. While an experiment was in progress, the chest

creaked occasionally, the equivalent of an earthquake. One model was

cast to represent overlap of strata near shore, like a coastal plain.

When squeezed, it made a group of overthrusts away from the piston

acting as shore rock.

In burial of strata there is a possibility whereby they wrinkle,

and wrinkle most in one direction, which piston pressure does not

imitate. That is the heating by burial and expansion or lengthening

of controlling layers. In a long basin like the Appalachians, the

wrinkling under expansion across the greatest length is easiest,

because the axis of stiffness is parallel to the long trough.

Transitions off the coastal line from one sediment to the next--sand

to mud, mud to lime--will be weaknesses to start bends when expansion

pressure takes place under burial along the layers separately heated.

These bends develop into wrinkles and the wrinkles, into propagated

folds, with the axis parallel to the initial change of weaknesses.

Expansion lengthwise on folds, once begun, may make long flat arches

pitching in one direction. This heating by burial distributes the

folding better and farther than pushing abutments, and makes initial

bends. All bottom strata heat and expand in all directions. The

direction of easiest yielding to a folding impulse is across the weak

transition belts. After that the motion is taken up by linear folds and

fractures in one direction.

The models, after continuous or intermittent squeezing, were removed

from the chest and sliced with a hot wire for sectioning and

photographing. In one, brittle, broken series of folds in a hard layer,

the model was taken apart on that layer and the surface photographed.

The crest of the folds showed jointing or regular cracks. One set

paralleled the fold axes as would be expected; the other set crossed

the slopes diagonally and in curves. These last indicated the strains

of a twisting nature on a single layer between a downfold and an upfold.

What makes the end thrust, or piston push, in nature? According to the

old idea, it was contraction of the inner earth by loss of heat. Willis

wrote that the basin sank, isostasy or deep flow was at right angles to

the length of the basin, and general contraction took effect by reason

of the deep flow. The deep flow was toward the lighter continent, from

which the sands were originally lost.

The recent notion that radioactivity heat is in the outer shell denies

contraction of the inner earth. Furthermore, I do not believe in a

shallow underlayer of lava fifty or less miles down and capable of

flowing horizontally under shifting weight. I do believe in a deep

underlayer of fluid 1,800 miles down, under a block-faulted crust.

This fluid core adjusted itself to the ocean-bottom blocks originally,

making the upright slices moving-down controllers of the Appalachian

basin. There is no proof that sediment weight did it. It is more likely

that igneous, or fire-made, lava, as the thick outer armor plate of

the globe erupted in acts of intrusion, lubricated the vertical slices.

Intrusions are under every sedimentary mountain range on earth. It is

more likely that an agelong up of ridge fault blocks and a down of the

basin fault blocks decided where the central continental basin should

be, all of it well within the permanent side ridges of North America.

For this was a continental mediterranean sea, and the warping of its

highland of Philadelphia and its basin of Cincinnati was a mere episode

in the 2,000 million year history of Atlantic and Pacific borders of

the continent. The sinking of the intracontinental sea, relative to

the staying up of the highlands, was a wave in the history of globe

and core. Erosion and deposition were results, not causes. They were

results of the volcanic history of the ever moving active mosaic of the

globe. The permanent North America remained high, relative to Atlantic

and Pacific deeps.

The folding of the sediments merges into intrusions of magma in the

southern Appalachians. Here arose the granite problem on a tremendous

scale, which is repeated in our Ascutney Mountain in Vermont. What

it was doing under the bottom of those vast fields of limestone from

Ohio to Illinois we have no idea. No more do we know what is doing

under the vast fields of lime and red ooze at the present bottoms of

the deep oceans. But we do know that fire-made rock squirts up under

all sea-laid sediments which anyone has ever studied on islands or

continents. This fire-made rock, solidified, has thickness and a

bottom. We do not know its thickness nor its bottom. We do know that

under it are big cracks 2,000 miles long rupturing it into volcano

systems. The conclusion is that the globe is mantled by a layer of

igneous matter which has spouted up cracks since more than 3,000

million years ago. How did this matter migrate by new intrusions,

to pull, push, heat, and wrinkle through 500 million years the dirt

accumulated in shallow Appalachian trenches from Alabama to Indiana? We

do not know.

The last of the Harvard experiments that I took part in concerned

melting up powders of basaltic minerals and rocks, letting them cool

down gradually, and then sectioning them for the polarizing microscope

to see how they resembled lavas. V. F. Marsters of the University of

Indiana helped me. Based on the European work of Doelter, Fouqué,

Michel-Lévy, and others, we used a French furnace with gas flame

blast and small crucibles of diatomaceous earth mixed with clay. The

specimen powders of crushed natural basalts, or mixtures of pyroxene,

feldspar and olivine, were kept glowing for forty to 150 hours, and

cooled either rapidly or slowly. The belief in those days was that slow

cooling was the main control of coarse crystallization. Quick or slow

cooling certainly does produce these effects in lava flows.

From quick cooling, we generally got radial bunches of crystals or

spherulites, in a glassy groundmass. From slow cooling, we got diabase

structure or coarser crystallization, with some openwork hollow

crystals. And there were little grains of magnetite and spinel. Much

time was wasted on furnace safety and methods, and on fire-punctured

crucibles of platinum, carbon, and graphite.

Nothing had been learned in 1900 about stirring, nor about gas as an

ingredient in basalt. It was not until years later, at the Hawaiian

Volcano Observatory, that Emerson proved that aa lava was made by

stirring a crucible. Aa is crystalline. Emerson got glassy lava by

quiet melting. No one has yet subjected lava to hydrogen blasts like

those of a Bessemer furnace, nor to other gases. There is a big field

here for imitating Mauna Loa and Etna fountains, and for critical

petrography of artificial basalts. Modern work has been concerned with

physical chemistry of limited mineral systems. So far as I know, no one

has mathematically synthesized natural rocks as an object in natural

history since the work of Carl Barus for the U. S. Geological Survey in

the nineties.

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