GLACIERS IN NEW YORK CITY
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GLACIERS IN NEW YORK CITY AN INTRODUCTION TO REGIONAL GEOLOGY In his book “Two Mile Time Machine,” Richard Alley explains that “To read the record of past climate shifts, we have to find the right history book” (p.11). Alley uses the chemical and physical evidence recorded in the layers of ancient ice to read the climate record. Rocks also record Earth’s history, and the rock record extends almost to the time of Earth’s formation 4.56 billion years ago. So you don’t need to go to Greenland with a drilling rig to read Earth’s history – you only need go to the park! In this laboratory, you will go into Central Park to learn to read the rock record and convince yourself (or not) that New York City was really buried under a thick slab of ice. Field Geology Outcrops, or exposures of bedrock at the surface of the Earth, are places where the rock record can be examined in situ (in place). Observation of rocks in outcrop is the most fundamental tool of geologists, allowing them to reconstruct the past. Field geologist Robert Compton wrote that, “The primary physical operation in studying outcrops is looking.” In an outcrop there is a lot to observe and geologists often talk about “getting your eye into it”, by which they mean seeing past the vegetation, deposits of the city, recent cracks or fractures in the rock etc… and seeing the layers upon layers of processes recorded by a parcel of the Earth. The goal of the field geologist is to (a) observe the rock and record “the facts”; and to (b) interpret the facts to infer processes. Fig. 1. Grand Canyon Rock Formation and Deformation in the Earth’s Crust If you have ever visited the Grand Canyon, you’ll remember that the walls of cliffs are layered (Fig 1). Geologists call this layering bedding and it is a primary feature that you’ll be looking for in the field. Each layer represents a deposit of sediment (carried by water or air) that became compacted and solidified to form Fig. 2. At left, the 1906 earthquake on the San Andreas sedimentary rock. The principle of Fault offsets a fence 8.5 feet in Point Reyes, California. superposition (young sediment is At right, frost action has created joints in the bedrock deposited on old sediment) states and erratic boulders dot the surface. that as you travel downwards in space, you are traveling backwards Page 1 of 9
in time - the same as with the ice cores. The nearly flat layering of the Grand Canyon can easily become warped and broken. When things get cold, they tend to break under stress, but when they are hot, they tend to stretch and bend (you’ll hear more about this in Professor Helfand’s lectures). Rocks are the same way. At the Earth’s cool surface, brittle deformation causes rocks to break. A fault is a break accompanied by motion (e.g. the San Andreas Fault), usually from an earthquake, whereas fractures or joints might simply be cracks due to freeze-thaw cycles (Fig. 2). Deeper in the Earth, increased pressure and temperature cause rocks to undergo ductile deformation and fold (Box 2). When the temperature rises sufficiently, the chemical constituents of sedimentary rocks react to create new minerals and new textures. This process of transformation is called metamorphosis. In this lab, you’ll see the Manhattan Schist, which is an example of a metamorphic rock (BOX I). BOX I: MANHATTAN SCHIST IN THE FIELD. (a) A typical Central Park outcrop of schist. The elongated layers of bedding or “foliation” are prominent in this image; it is highly folded and weathered such that some layers stick out more than others. (b) This schist is typical of outcrops in Inwood Park. Metamorphic minerals called garnets (the red-colored knobs) and mica (shiny silver platy flecks) are prominent in this image. The highly deformed and folded structure is still evident. Both images contain a familiar “object for scale” (a Swiss army knife and a dime respectively). All pictures and sketches from the field require such a reference mark – otherwise it isn’t clear if the image is the size of your fingernail or a mountainside. Page 2 of 9
The Manhattan Schist – The bedrock of New York City Most of Manhattan is underlain by the Manhattan Schist (BOX I), the bedrock that supports New York’s towering skyscrapers. Have you ever wondered why there are no tall buildings in Greenwich Village while midtown and downtown are full of skyscrapers? Manhattan schist is found 18 feet below the surface in Times Square and 260 feet below in Greenwich Village. Where the schist dips down skyscrapers are much more difficult to construct because there is no bedrock to provide structural support. Greenwich Village remains a low-lying neighborhood, but skyscrapers dominate midtown and the financial district where schist lies close to the surface. Similarly, the supports for the George Washington Bridge are on Manhattan Schist. To understand the history of New York City, you have to start 500 million (5x108) years ago in the Paleozoic Era. Figure 3: A map of bedrock geology reveals the patterns and structures made by the rock units in the Earth’s crust. This map is presented either in map view (or “birds eye” view) (a), or it can give a cross sectional view (b). Because each view is only a two- dimensional slice, we need both views to understand three-dimensional rock structures. X Y X New Jersey New York Palisades Sill (Triassic Volcanic Rock) Y Manhattan Schist A B Page 3 of 9
Figure 4 gives a sense of the vast history of our planet. In this lab you’ll be looking at rocks that are 500 million years old, first deposited before the evolution of plants. Even so, the rocks you’ll see only represent the last 10% of Earth’s history! These pages will describe three important events in the city during that time that will set the stage for what you’ll be seeing on your field excursion: the Taconic Orogeny, the opening of the Atlantic Ocean, and the glacial episodes of the recent geological past, which you’ll learn about Fig 4. Timing of some events in Earth history. in lecture. The Taconic Orogeny New York City bedrock began as muds and sands deposited 500 million years ago in an ocean – the Iapetus Ocean – off the coast of what is now North America. These deposits were buried and compacted, and eventually turned into sedimentary rock. Due to plate tectonics (for more info see http://pubs.usgs.gov/publications/text/dynamic.html), an earlier Atlantic Ocean (the Iapetus Ocean) closed as a massive chain of islands (analogous to Japan) collided into North America between 480-440 million years ago. The once flat-lying sediments became folded and deformed and were buried deep within a mountain range called the Taconic Mountains, which were a massive range like the Himalayas. Beneath these ancient peaks, the sedimentary rocks were heated, compressed, and metamorphosed to create the Manhattan Schist (Box I). A mountain building event such as this is called an orogeny. During the last major collision at 310-250 million years ago, all of the continents came together to create one supercontinent called Pangea, meaning “all Earth” (Fig. 5). Where are these mighty peaks now you might ask? As far as mountains are concerned, if you aren’t on your way up, you are on your way down. After the collision ended the once high and mighty Taconic Mountains eroded away and eventually exposed their ancient metamorphosed core, including the Manhattan Schist, for your viewing pleasure. Page 4 of 9
BOX II: BRITTLE VS DUCTILE DEFORMATION We all know that rocks near the surface of the Earth behave in a brittle manner: they fracture and fault in response to stress. As we go deeper in the Earth the strength of these rocks initially increases. At a depth of about 15 km we reach a point called the brittle-ductile transition zone. Below this point rock strength decreases because the temperature is higher. The rocks behave in a ductile manner; they fold and deform like stiff taffy. Page 5 of 9
The Opening of the Atlantic Ocean Pangea began to “rift” apart ~200 million years ago at the end of the Triassic Period – the beginning of the age of dinosaurs – when the Americas began to pull apart from Europe and Africa, and again forming mountains and valleys (rifting creates long linear valleys Figure 5 with mountain ranges on each side – Nevada is composed entirely of long rift valleys with Fig. 5 mountains on each side). Manhattan lies within this ancient rift valley, which filled with sediment from the mountains. Virtually all large rifts on the Earth’s surface have volcanoes. When continents rift apart, hot molten rock (magma) from the Earth’s interior fills the gap in the form of volcanoes and dikes. The cliffs across the Hudson from Manhattan are composed of a great block of cooled magma – the Palisades – that forced its way into the sedimentary layers in the rift during the break-up of Pangea. In the field, you might also see smaller dikes cross-cutting the bedding in the Manhattan Schist. Since the break-up of Pangea there have been no more orogenies in New York. Running water and moving ice have eroded the mountains and valleys. The Palisades and the Manhattan Schist are exposed today because they are harder and more difficult to erode than the surrounding sediments. In the field, you’ll see evidence of ancient orogenies and rifting. In summary, these geologic processes - orogeny, erosion, and rifting - created the rocks in Manhattan that you will see on your field excursion. The Glacial Age of the Last 450 Thousand Years In 1815, the Swiss mountaineer Jean-Pierre Perraudin communicated to the scientific community a radical notion: Having long ago observed marks or scars occurring on hard rocks which do not weather, I finally decided, after going near the glaciers, that they had been made by the pressure or weight of these masses, of which I find traces at least as far as Champsec. This makes me think that glaciers filled in the past the entire Val de Bagnes, and I am ready to demonstrate this fact to the incredulous people by the obvious proof of comparing these marks with those uncovered by glaciers at present. - Quote excerpted from “Ice Ages” by Imbrie and Imbrie You have read in Alley’s book how ice cores from Greenland and Antarctica record the last seven glacial episodes in their d18O chemistry, extending back in time nearly half a million years. The ice core record, however, was a relative latecomer in our understanding of our planet’s glacial past. Evidence that ice had previously reached low latitudes was recognized by Page 6 of 9
Europeans, such as Perraudin in the 1800s, before the discovery of the atom and long before the concept of isotopic fractionation between 18O and 16O. Among the many achievements of Charles Darwin was his recognition that certain sediment deposits in England, and the U-shaped valleys of Scotland, were formed by glaciers. Figure 6 shows an artist’s representation of the ice cover during the last glacial maximum, which ended about 12,000 years ago. We know that the ice extended all the way to New York. (In this sense, the idea in the movie The Day After Tomorrow, that the ice can reach New York is not farfetched). To understand the physical signature of the ice ages, one needs to understand the physics of ice. Fresh snow is fluffy and loose (density ~0.14 g/cm3). Like mud and sand transform into harder sedimentary rocks under pressure, snow too becomes compacted to form firn, or very dense snow (density ~0.8 g/cm3). Further compaction results in the dense crystalline mineral ice. Glacial ice has a density of ~ 0.9 g/cm3. Ice can be folded and faulted under stress and pressure just like the rocks that made the Taconic Mountains. When enough pressure causes the ice to flow and deform, Figure 6 it is called a glacier. Figure 7 shows a cross section through a glacier. Snow is replenished in the winter in the zone of accumulation and snow is lost in the summertime in the zone of ablation. The mass balance that is struck between these two processes determines whether the glacier will advance or retreat (get smaller). Climate is the main influence on mass balance. A glacier “retreats” when it melts faster than it advances. Figure 7 Glacial Landforms Large and Small The first step in glacial erosion is rock failure. Rock failure can occur as the growth of pre- existing cracks or the formation of new cracks. Cracks form at weaknesses within the rock. When water that has infiltrated into cracks freezes into ice it expands up to 10% in volume (again, because ice is less dense than water – see BOX III). The expansion forces the crack to widen, a process known as frost action. The other significant erosional process is abrasion. Debris lodged in the ice grinds into the bedrock and scars the rock in way that is consistent with how coarse the debris is (just as with sandpaper on wood). This grinding can leave a finely polished surface or long grooves in the bedrock called striations (Appendix III). Glacial striae are linear scratches in the bedrock caused by ice and debris flow. They can occur at all scales, from microscopic scratches to centimeter wide grooves, to foot wide troughs. (For example, a glacial trough might contain Page 7 of 9
BOX III: HOW GLACIERS FLOW smaller grooves within it, and these are likely to have scratches that can only be seen with a microscope – they are all examples of glacial striae). Glacial striae are cut into the existing bedrock in an orientation consistent with the direction of ice flow. For this reason, they are often at an oblique angle to the bedding. [Note: bedding - the sedimentary For most compounds, including rock, solids are layering in the bedrock - can look denser than liquids. Because of this property, high “grooved” as well due to differing pressures make rocks less likely to melt because rates of erosion. Be careful!] pressure pushes atoms together. The compound H2O possesses a very peculiar property: the liquid form If the glacier is no longer present, (water) is more dense than the solid (ice) – you know striations can be used to determine this because ice floats. Application of pressure causes the direction of ice flow. ice to melt, and pressure release causes refreezing. Push two ice cubes together with force and then let go Unlike rivers or streams, glaciers can – they stick! move any size particle. Large boulders left behind by melting A glacier works in the same way: high pressures at the glaciers such as this are termed base cause the base to flow along at rates of a e r r a t i c s because they bear no millimeter to a meter per day. While ice at the base relation to the surrounding bedrock. flows and deforms in a ductile manner, ice at the Also, while streams erode bedrock to surface fractures and creates crevasses, or brittle create “V-shaped” valleys, glaciers deformation. create broad erosional features called U-shaped valleys (Fig. 8) and fjords. The relationship between U-shaped valleys and glaciers were first noticed in high mountains containing mountain glaciers You will be looking for glacial striations and erratics during your lab exercise. The end of a glacier is called the For the same reasons, glacial ice melts when it is terminus and its position reflects the pressurized against a bump in the bedrock. On the mass balance of the glacier in other side of the bump, the ice refreezes and plucks response to climate. While the chunks off of the bedrock. The net result is a glacier is advancing, it works like a landform called a roche moutoneé that is rounded and plow, pushing everything in its path. smoothed on one side, and angular, blocky and steep When the glacier retreats during a on the other. These forms occur in all sizes – from warming period, it leaves its load of small outcrops to mountain range shapes. Some of debris and creates a landform called you will be looking for these features in the field. a terminal moraine (Fig. 8, and see G l o s s a r y ). The sediment of a Page 8 of 9
moraine is called till (a Scottish word for rocky soil). Till units are not size-sorted the way a stream deposits are – with bigger particles falling out first and fine particles settling out later on. Rocks carried by glaciers do not become sorted by mass as they travel down-slope (remember, glaciers have unlimited carrying capacity). Mapping the farthest advance of an ice front simply becomes a matter of mapping the limit of till deposits which make up the terminal moraines. You’ll do this too! The boulder field (Wind River, WY) at left below is part of the terminal moraine of the last ice sheet that covered North America. “Small” glaciers associated with high mountains also make U-shaped valleys and terminal moraines as shown at the base of Teton Glacier, WY (at right below). Figure 8 Page 9 of 9
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