{"id":447,"date":"2019-06-11T14:50:41","date_gmt":"2019-06-11T14:50:41","guid":{"rendered":"https:\/\/opentextbc.ca\/physicalgeology2ed\/chapter\/10-3-geological-renaissance-of-the-mid-20th-century\/"},"modified":"2021-12-08T16:58:15","modified_gmt":"2021-12-08T16:58:15","slug":"10-3-geological-renaissance-of-the-mid-20th-century","status":"publish","type":"chapter","link":"https:\/\/opentextbc.ca\/physicalgeology2ed\/chapter\/10-3-geological-renaissance-of-the-mid-20th-century\/","title":{"raw":"10.3 Geological Renaissance of the Mid-20th Century","rendered":"10.3 Geological Renaissance of the Mid-20th Century"},"content":{"raw":"As the mineral magnetite (Fe<sub>3<\/sub>O<sub>4<\/sub>) crystallizes from magma, it becomes magnetized with an orientation parallel to that of Earth's magnetic field at that time. This is called <strong>[pb_glossary id=\"1617\"]remnant magnetism[\/pb_glossary]<\/strong>. Rocks like basalt, which cool from a high temperature and commonly have relatively high levels of magnetite (up to 1 or 2%), are particularly susceptible to being magnetized in this way, but even sediments and sedimentary rocks, as long as they have small amounts of magnetite, will take on remnant magnetism because the magnetite grains gradually become reoriented following deposition. By studying both the horizontal and vertical components of the remnant magnetism, one can tell not only the direction to magnetic north at the time of the rock's formation, but also the latitude where the rock formed relative to magnetic north.\r\n\r\nIn the early 1950s, a group of geologists from Cambridge University, including Keith Runcorn, Ted Irving,[footnote]Ted Irving later set up a paleomagnetic lab at the Geological Survey of Canada in Sidney, B.C., and did a great deal of important work on understanding the geology of western North America.[\/footnote]\u00a0and several others, started looking at the remnant magnetism of Phanerozoic British and European volcanic rocks, and collecting <strong>[pb_glossary id=\"1618\"]paleomagnetic[\/pb_glossary]<\/strong> data. They found that rocks of different ages sampled from generally the same area showed quite different apparent magnetic pole positions (Figure 10.3.1). They initially assumed that this meant that Earth's magnetic field had, over time, departed significantly from its present position\u2014which is close to the rotational pole.\r\n\r\n[caption id=\"attachment_433\" align=\"aligncenter\" width=\"700\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131.png\"><img class=\"wp-image-433\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131.png\" alt=\"\" width=\"700\" height=\"348\" \/><\/a> Figure 10.3.1 Apparent polar-wandering paths (APWP) for Eurasia and North America. The view is from the North Pole (black dot) looking down. The outer circle is the equator. In the diagram to the right the curve locations have been corrected taking continental drift into account.[\/caption]\r\n\r\nThe curve defined by the paleomagnetic data was called a <strong>[pb_glossary id=\"1619\"]polar wandering path[\/pb_glossary]<\/strong> because Runcorn and his students initially thought that their data represented actual movement of the magnetic poles (since geophysical models of the time suggested that the magnetic poles did not need to be aligned with the rotational poles). We now know that the magnetic data define movement of continents, and <em>not<\/em> of the magnetic poles, so we call it an <em>apparent<\/em> polar wandering path (APWP).\r\n<div class=\"textbox textbox--examples\"><header class=\"textbox__header\">\r\n<p class=\"textbox__title\">What is a polar wandering path?<a id=\"retfig10.3.2\"><\/a><\/p>\r\n\r\n<\/header>\r\n<div class=\"textbox__content\">[caption id=\"attachment_434\" align=\"alignright\" width=\"400\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0151.png\"><img class=\"wp-image-434\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0151.png\" alt=\"The magnetic orientation of rocks in Europe from 500 Ma to the present. Image description available\" width=\"400\" height=\"439\" \/><\/a> Figure 10.3.2 <a href=\"#fig10.3.2\">[Image Description]<\/a>[\/caption]At around 500 Ma, what we now call Europe was south of the equator, and so European rocks formed then would have acquired an upward-pointing magnetic field orientation (see Figure 9.3.2 and Figure 10.3.2). Between then and now, Europe gradually moved north, and the rocks forming at various times acquired steeper and steeper <em>downward-pointing<\/em> magnetic orientations.When researchers evaluated magnetic data in this way in the 1950s, they plotted where the North Pole would have appeared to be based on the magnetic data and assumed that the continent was always where it is now. That means that the 500 Ma \u201capparent\u201d north pole would have been somewhere in the South Pacific, and that over the following 500 million years it would have gradually moved north.Of course we now know that the magnetic poles don\u2019t move around much (although polarity reversals do take place) and that the reason Europe had a magnetic orientation characteristic of the southern hemisphere is that it was in the southern hemisphere at 500 Ma.Runcorn and colleagues soon extended their work to North America, and this also showed <em>apparent<\/em> polar wandering, but the results were not consistent with those from Europe. For example, the 200 Ma pole for North America plotted somewhere in China, while the 200 Ma pole for Europe plotted in the Pacific Ocean. Since there could only have been one pole position at 200 Ma, this evidence strongly supported the idea that North America and Europe had moved relative to each other since 200 Ma. Subsequent paleomagnetic work showed that South America, Africa, India, and Australia also have unique polar wandering curves. In 1956, Runcorn changed his mind and became a proponent of continental drift.This paleomagnetic work of the 1950s was the first new evidence in favour of continental drift, and it led a number of geologists to start thinking that the idea might have some merit. Nevertheless, for a majority of geologists working on global geology at the time, this type of evidence was not sufficiently convincing to get them to change their views.<\/div>\r\n<\/div>\r\nDuring the 20th century, our knowledge and understanding of the ocean basins and their geology increased dramatically. Before 1900, we knew virtually nothing about the bathymetry and geology of the oceans. By the end of the 1960s, we had detailed maps of the topography of the ocean floors, a clear picture of the geology of ocean floor sediments and the solid rocks underneath them, and almost as much information about the geophysical nature of ocean rocks as of continental rocks.\r\n\r\nUp until about the 1920s, ocean depths were measured using weighted lines dropped overboard. In deep water this is a painfully slow process and the number of soundings in the deep oceans was probably fewer than 1,000. That is roughly one depth sounding for every 350,000 square kilometres of the ocean. To put that in perspective, it would be like trying to describe the topography of British Columbia with elevation data for only a half a dozen points! The voyage of the <em>Challenger<\/em> in 1872 and the laying of trans-Atlantic cables had shown that there were mountains beneath the seas, but most geologists and oceanographers still believed that the oceans were essentially vast basins with flat bottoms, filled with thousands of metres of sediments.\r\n\r\nFollowing development of acoustic depth sounders in the 1920s (Figure 10.3.3), the number of depth readings increased by many orders of magnitude, and by the 1930s, it had become apparent that there were major mountain chains in all of the world's oceans. During and after World War II, there was a well-organized campaign to study the oceans, and by 1959, sufficient bathymetric data had been collected to produce detailed maps of all the oceans (Figure 10.3.4).\r\n\r\n[caption id=\"attachment_435\" align=\"aligncenter\" width=\"600\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0171.png\"><img class=\"wp-image-435\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0171.png\" alt=\"&quot;&quot;\" width=\"600\" height=\"267\" \/><\/a> Figure 10.3.3 Depiction of a ship-borne acoustic depth sounder. The instrument emits a sound (black arcs) that bounces off the sea floor and returns to the surface (white arcs). The travel time is proportional to the water depth.[\/caption]\r\n\r\n[caption id=\"attachment_436\" align=\"aligncenter\" width=\"700\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4.jpg\"><img class=\"wp-image-436\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4.jpg\" alt=\"\" width=\"700\" height=\"467\" \/><\/a> Figure 10.3.4 Ocean floor bathymetry (and continental topography). Inset (a): the mid-Atlantic ridge, (b): the Newfoundland continental shelf, (c): the Nazca trench adjacent to South America, and (d): the Hawaiian Island chain.[\/caption]\r\n\r\nThe important physical features of the ocean floor are:\r\n<ul>\r\n \t<li>Extensive linear ridges (commonly in the central parts of the oceans) with water depths in the order of 2,000 to 3,000 m (Figure 10.3.4, inset a)<\/li>\r\n \t<li>Fracture zones perpendicular to the ridges (inset a)<\/li>\r\n \t<li>Deep-ocean plains at depths of 5,000 to 6,000 m (insets a and d)<\/li>\r\n \t<li>Relatively flat and shallow continental shelves with depths under 500 m (inset b)<\/li>\r\n \t<li>Deep trenches (up to 11,000 m deep), most near the continents (inset c)<\/li>\r\n \t<li>Seamounts and chains of seamounts (inset d)<\/li>\r\n<\/ul>\r\n<strong>[pb_glossary id=\"1620\"]Seismic reflection sounding[\/pb_glossary]<\/strong> involves transmitting high-energy sound bursts and then measuring the echos with a series of geophones towed behind a ship. The technique is related to <em>acoustic sounding<\/em> as described above; however, much more energy is transmitted and the sophistication of the data processing is much greater. As the technique evolved, and the amount of energy was increased, it became possible to <em>see through<\/em> the sea-floor sediments and map the bedrock topography and crustal thickness. Hence sediment thicknesses could be mapped, and it was soon discovered that although the sediments were up to several thousands of metres thick near the continents, they were relatively thin \u2014 or even non-existent \u2014 in the ocean ridge areas (Figure 10.3.5). The seismic studies also showed that the crust is relatively thin under the oceans (5 km to 6 km) compared to the continents (30 km to 60 km) and geologically very consistent, composed almost entirely of basalt.\r\n\r\n[caption id=\"attachment_437\" align=\"aligncenter\" width=\"800\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments.png\"><img class=\"wp-image-437\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments.png\" alt=\"\" width=\"800\" height=\"163\" \/><\/a> Figure 10.3.5 Topographic section at an ocean ridge based on reflection seismic data. Sediments are not thick enough to be detectable near the ridge, but get thicker on either side. The diagram represents approximately 50 km width, and has a 10x vertical exaggeration.[\/caption]\r\n\r\nIn the early 1950s, Edward Bullard, who spent time at the University of Toronto but is mostly associated with Cambridge University, developed a probe for measuring the flow of heat from the ocean floor. Bullard and colleagues found the rate to be higher than average along the ridges, and lower than average in the trench areas. Although Bullard was a plate-tectonics sceptic, these features were interpreted to indicate that there is convection within the mantle \u2014 the areas of high heat flow being correlated with upward convection of hot mantle material, and the areas of low heat flow being correlated with downward convection.\r\n\r\nWith developments of networks of seismographic stations in the 1950s, it became possible to plot the locations <em>and<\/em> depths of both major and minor earthquakes with great accuracy. It was found that there is a remarkable correspondence between earthquakes and both the mid-ocean ridges and the deep ocean trenches. In 1954 Gutenberg and Richter showed that the ocean-ridge earthquakes were all relatively shallow, and confirmed what had first been shown by Benioff in the 1930s \u2014 that earthquakes in the vicinity of ocean trenches were both shallow and deep, but that the deeper ones were situated progressively farther inland from the trenches (Figure 10.3.6).<a id=\"retfig10.3.6\"><\/a>\r\n\r\n[caption id=\"attachment_438\" align=\"aligncenter\" width=\"800\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes.png\"><img class=\"wp-image-438\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes.png\" alt=\"\" width=\"800\" height=\"182\" \/><\/a> Figure 10.3.6 Cross-section through the Aleutian subduction zone with a depiction of the increasing depth of earthquakes \u201cinshore\u201d from the trench. <a href=\"#fig10.3.6\">[Image Description]<\/a>[\/caption]In the 1950s, scientists from the Scripps Oceanographic Institute in California persuaded the U.S. Coast Guard to include magnetometer readings on one of their expeditions to study ocean floor topography. The first comprehensive magnetic data set was compiled in 1958 for an area off the coast of B.C. and Washington State. This survey revealed a bewildering pattern of low and high magnetic intensity in sea-floor rocks (Figure 10.3.7). When the data were first plotted on a map in 1961, nobody understood them \u2014 not even the scientists who collected them. Although the patterns made even less sense than the stripes on a zebra, many thousands of kilometres of magnetic surveys were conducted over the next several years.\r\n\r\n[caption id=\"attachment_439\" align=\"alignright\" width=\"350\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason.png\"><img class=\"wp-image-439\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason.png\" alt=\"\" width=\"350\" height=\"282\" \/><\/a> Figure 10.3.7 Pattern of sea-floor magnetism off of the west coast of British Columbia and Washington.[\/caption]\r\n\r\nThe wealth of new data from the oceans began to significantly influence geological thinking in the 1960s. In 1960, Harold Hess, a widely respected geologist from Princeton University, advanced a theory with many of the elements that we now accept as <strong>[pb_glossary id=\"1356\"]plate tectonics[\/pb_glossary]<\/strong>. He maintained some uncertainty about his proposal however, and in order to deflect criticism from mainstream geologists, he labelled it <em>geopoetry<\/em>. In fact, until 1962, Hess didn't even put his ideas in writing\u2014except internally to the U.S. Navy (which funded his research)\u2014but presented them mostly in lectures and seminars. Hess proposed that new sea floor was generated from mantle material at the ocean ridges, and that old sea floor was dragged down at the ocean trenches and re-incorporated into the mantle. He suggested that the process was driven by mantle convection currents, rising at the ridges and descending at the trenches (Figure 10.3.8). He also suggested that the less-dense continental crust did not descend with oceanic crust into trenches, but that colliding land masses were thrust up to form mountains. Hess's theory formed the basis for our ideas on <strong>[pb_glossary id=\"1621\"]sea-floor spreading[\/pb_glossary]<\/strong> and <strong>[pb_glossary id=\"1622\"]continental drift[\/pb_glossary]<\/strong><strong>,<\/strong> but it did not deal with the concept that the crust is made up of specific <strong>[pb_glossary id=\"1624\"]plates[\/pb_glossary]<\/strong>. Although the Hess model was not roundly criticized, it was not widely accepted (especially in the U.S.), partly because it was not well supported by hard evidence.\r\n\r\n[caption id=\"attachment_440\" align=\"aligncenter\" width=\"800\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model.png\"><img class=\"wp-image-440\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model.png\" alt=\"\" width=\"800\" height=\"265\" \/><\/a> Figure 10.3.8 A representation of Harold Hess\u2019s model for sea-floor spreading and subduction.[\/caption]\r\n\r\nCollection of magnetic data from the oceans continued in the early 1960s, but still nobody could explain the origin of the zebra-like patterns. Most assumed that they were related to variations in the composition of the rocks\u2014such as variations in the amount of magnetite\u2014as this is a common explanation for magnetic variations in rocks of the continental crust. The first real understanding of the significance of the striped anomalies was the interpretation by Fred Vine, a Cambridge graduate student. Vine was examining magnetic data from the Indian Ocean and, like others before, he noted the symmetry of the magnetic patterns with respect to the oceanic ridge.\r\n\r\nAt the same time, other researchers, led by groups in California and New Zealand, were studying the phenomenon of reversals in Earth's magnetic field. They were trying to determine when such reversals had taken place over the past several million years by analyzing the magnetic characteristics of hundreds of samples from basaltic flows. As discussed in Chapter 9, it is evident that Earth\u2019s magnetic field becomes weakened periodically and then virtually non-existent, before becoming re-established with the reverse polarity. During periods of reversed polarity, a compass would point south instead of north.\r\n\r\nThe time scale of magnetic reversals is irregular. For example, the present \"normal\" event, known as the Bruhnes magnetic chron, has persisted for about 780,000 years. This was preceded by a 190,000-year reversed event; a 50,000-year normal event known as Jaramillo; and then a 700,000-year reversed event (see Figure 9.3.3).\r\n\r\nIn a paper published in September 1963, Vine and his PhD supervisor Drummond Matthews proposed that the patterns associated with ridges were related to the magnetic reversals, and that oceanic crust created from cooling basalt during a <em>normal<\/em> event would have polarity aligned with the present magnetic field, and thus would produce a positive anomaly (a black stripe on the sea-floor magnetic map), whereas oceanic crust created during a <em>reversed<\/em> event would have polarity opposite to the present field and thus would produce a negative magnetic anomaly (a white stripe). The same idea had been put forward a few months earlier by Lawrence Morley, of the Geological Survey of Canada; however, his papers submitted earlier in 1963 to <em>Nature<\/em> and <em>The Journal of Geophysical Research<\/em> were rejected. Many people refer to the idea as the Vine-Matthews-Morley (VMM) hypothesis.\r\n\r\nVine, Matthews, and Morley were the first to show this type of correspondence between the relative widths of the stripes and the periods of the magnetic reversals. The VMM hypothesis was confirmed within a few years when magnetic data were compiled from spreading ridges around the world. It was shown that the same general magnetic patterns were present straddling each ridge, although the widths of the anomalies varied according to the spreading rates characteristic of the different ridges. It was also shown that the patterns corresponded with the chronology of Earth's magnetic field reversals. This global consistency provided strong support for the VMM hypothesis and led to rejection of the other explanations for the magnetic anomalies.\r\n\r\nIn 1963, J. Tuzo Wilson of the University of Toronto proposed the idea of a <strong>[pb_glossary id=\"1160\"]mantle plume[\/pb_glossary]<\/strong> or <strong>[pb_glossary id=\"1625\"]hot spot[\/pb_glossary]<\/strong>\u2014a place where hot mantle material rises in a stationary and semi-permanent plume, and affects the overlying crust. He based this hypothesis partly on the distribution of the Hawaiian and Emperor Seamount island chains in the Pacific Ocean (Figure 10.3.9). The volcanic rock making up these islands gets progressively younger toward the southeast, culminating with the island of Hawaii itself, which consists of rock that is almost all younger than 1 Ma. Wilson suggested that a stationary plume of hot upwelling mantle material is the source of the Hawaiian volcanism, and that the ocean crust of the Pacific Plate is moving toward the northwest over this hot spot. Near the Midway Islands, the chain takes a pronounced change in direction, from northwest-southeast for the Hawaiian Islands and to nearly north-south for the Emperor Seamounts. This change is widely ascribed to a change in direction of the Pacific Plate moving over the stationary mantle plume, but a more plausible explanation is that the Hawaiian mantle plume has not actually been stationary throughout its history, and in fact moved at least 2,000 km south over the period between 81 and 45 Ma.[footnote]J. A. Tarduno et al., 2003, The Emperor Seamounts: Southward Motion of the Hawaiian Hotspot Plume in Earth\u2019s Mantle,\u00a0Science\u00a0301\u00a0(5636): 1064\u20131069.[\/footnote]\r\n\r\n[caption id=\"attachment_441\" align=\"aligncenter\" width=\"784\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312.png\"><img class=\"wp-image-441 size-full\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312.png\" alt=\"\" width=\"784\" height=\"573\" \/><\/a> Figure 10.3.9 The ages of the Hawaiian Islands and the Emperor Seamounts in relation to the location of the Hawaiian mantle plume.[\/caption]\r\n\r\n<div class=\"textbox textbox--exercises\"><header class=\"textbox__header\">\r\n<p class=\"textbox__title\">Exercise 10.2 Volcanoes and the Rate of Plate Motion<\/p>\r\n\r\n<\/header>\r\n<div class=\"textbox__content\">\r\n\r\nThe Hawaiian and Emperor volcanoes shown in Figure 10.3.9 are listed in the table below along with their ages and their distances from the centre of the mantle plume under Hawaii (the Big Island).\r\n<table border=\"1\"><caption>Ages of Hawaiian and Emperor volcanoes and their distances from the centre of the mantle plume. Calculate their rate of movement in centimetres per year.\u00a0<\/caption>\r\n<tbody>\r\n<tr>\r\n<th scope=\"col\">Island<\/th>\r\n<th scope=\"col\">Age<\/th>\r\n<th scope=\"col\">Distance<\/th>\r\n<th scope=\"col\">Rate<\/th>\r\n<\/tr>\r\n<tr>\r\n<td>Hawaii<\/td>\r\n<td>0 Ma<\/td>\r\n<td>0 km<\/td>\r\n<td>-<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>Necker<\/td>\r\n<td>10.3 Ma<\/td>\r\n<td>1,058 km<\/td>\r\n<td>10.2 cm\/y<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>Midway<\/td>\r\n<td>27.7 Ma<\/td>\r\n<td>2,432 km<\/td>\r\n<td><\/td>\r\n<\/tr>\r\n<tr>\r\n<td>Koko<\/td>\r\n<td>48.1 Ma<\/td>\r\n<td>3,758 km<\/td>\r\n<td><\/td>\r\n<\/tr>\r\n<tr>\r\n<td>Suiko<\/td>\r\n<td>64.7 Ma<\/td>\r\n<td>4,860 km<\/td>\r\n<td><\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\nPlot the data on the graph provided here, and use the numbers in the table to estimate the rates of plate motion for the Pacific Plate in cm\/year. (The first two are plotted for you.)\r\n\r\n<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0331.png\"><img class=\"aligncenter wp-image-442\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0331.png\" alt=\"A blank graph. Distance (in kilometres) on y-axis. Age (Ma) on x-axis\" width=\"600\" height=\"403\" \/><\/a>\r\n\r\nSee Appendix 3 for <a href=\"\/physicalgeology2ed\/back-matter\/appendix-3-answers-to-exercises\/#exercisea10.2\">Exercise 10.2 answers<\/a>.\r\n\r\n<\/div>\r\n<\/div>\r\nThere is evidence of many such mantle plumes around the world (Figure 10.3.10). Most are within the ocean basins\u2014including places like Hawaii, Iceland, and the Galapagos Islands\u2014but some are under continents. One example is the Yellowstone hot spot in the west-central United States, and another is the one responsible for the Anahim Volcanic Belt in central British Columbia. It is evident that mantle plumes are very long-lived phenomena, lasting for at least tens of millions of years, possibly for hundreds of millions of years in some cases.\r\n\r\n[caption id=\"attachment_443\" align=\"aligncenter\" width=\"884\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots.png\"><img class=\"wp-image-443 size-full\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots.png\" alt=\"\" width=\"884\" height=\"514\" \/><\/a> Figure 10.3.10 Mantle plume locations. Selected Mantle plumes: 1: Azores, 3: Bowie, 5: Cobb, 8: Eifel, 10: Galapagos, 12: Hawaii, 14: Iceland, 17: Cameroon, 18: Canary, 19: Cape Verde, 35: Samoa, 38: Tahiti, 42: Tristan, 44: Yellowstone, 45: Anahim[\/caption]\r\n\r\nAlthough oceanic spreading ridges appear to be curved features on Earth's surface, in fact the ridges are composed of a series of straight-line segments, offset at intervals by faults perpendicular to the ridge (Figure 10.3.11). In a paper published in 1965, Tuzo Wilson termed these features <strong>[pb_glossary id=\"1626\"]transform faults[\/pb_glossary]<\/strong>. He described the nature of the motion along them, and showed why there are earthquakes only on the section of a transform fault between two adjacent ridge segments. The San Andreas Fault in California is a very long transform fault that links the southern end of the Juan de Fuca spreading ridge to the East Pacific Rise spreading ridges situated in the Gulf of California (see Figure 10.4.9). The Queen Charlotte Fault, which extends north from the northern end of the Juan de Fuca spreading ridge (near the northern end of Vancouver Island) toward Alaska, is also a transform fault.\r\n\r\n[caption id=\"attachment_444\" align=\"aligncenter\" width=\"800\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform.png\"><img class=\"wp-image-444\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform.png\" alt=\"\" width=\"800\" height=\"316\" \/><\/a> Figure 10.3.11 A part of the mid-Atlantic ridge near the equator. The double white lines are spreading ridges. The solid white lines are fracture zones. As shown by the yellow arrows, the relative motion of the plates on either side of the fracture zones can be similar (arrows pointing the same direction) or opposite (arrows pointing opposite directions). Transform faults (red lines) are in between the ridge segments, where the yellow arrows point in opposite directions.[\/caption]\r\n\r\nIn the same 1965 paper, Wilson introduced the idea that the crust can be divided into a series of rigid plates, and thus he is responsible for the term <strong>[pb_glossary id=\"1356\"]plate tectonics[\/pb_glossary]<\/strong>.\r\n<div class=\"textbox textbox--exercises\"><header class=\"textbox__header\">\r\n<p class=\"textbox__title\">Exercise 10.3 Paper transform fault model<\/p>\r\n\r\n<\/header>\r\n<div class=\"textbox__content\">\r\n\r\n[caption id=\"attachment_445\" align=\"aligncenter\" width=\"950\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model.png\"><img class=\"wp-image-445\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model.png\" alt=\"\" width=\"950\" height=\"379\" \/><\/a> Figure 10.3.12[\/caption]\r\n\r\nTuzo Wilson used a paper model, a little bit like the one shown here, to explain transform faults to his colleagues. To use this model either print this page or download the image above and print that, then cut around the outside, and then slice along the line A-B (the fracture zone) with a sharp knife. Fold down the top half where shown, and then pinch together in the middle. Do the same with the bottom half.\r\n\r\n[caption id=\"attachment_446\" align=\"alignright\" width=\"400\"]<a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411.jpg\"><img class=\"wp-image-446 size-full\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411.jpg\" alt=\"\" width=\"400\" height=\"266\" \/><\/a> Figure 10.3.13[\/caption]\r\n\r\nWhen you\u2019re done, you should have something like the example shown on Figure 10.3.13, with two folds of paper extending underneath. Find someone else to pinch those folds with two fingers just below each ridge crest, and then gently pull apart where shown. As you do, the oceanic crust will emerge from the middle, and you\u2019ll see that the parts of the fracture zone between the ridge crests will be moving in opposite directions (this is the transform fault) while the parts of the fracture zone outside of the ridge crests will be moving in the same direction. You\u2019ll also see that the oceanic crust is being magnetized as it forms at the ridge. The magnetic patterns shown are accurate, and represent the last 2.5 Ma of geological time.\r\n\r\nThere are other versions of this model available here: <a href=\"https:\/\/web.viu.ca\/earle\/transform-model\/\">Paper Models of Transform Faults<\/a>.[footnote]For more information see: Earle, S., 2004,\u00a0<em>A simple paper model of a transform fault at a spreading ridge<\/em>,\u00a0J. Geosc. Educ.\u00a0V. 52, p. 391-2.[\/footnote]\r\n\r\nSee Appendix 3 for <a href=\"\/physicalgeology2ed\/back-matter\/appendix-3-answers-to-exercises\/#exercisea10.3\">Exercise 10.3 answers<\/a>.\r\n\r\n<\/div>\r\n<\/div>\r\n<div>\r\n<h3>Image Descriptions<\/h3>\r\n<strong id=\"fig10.8\"><a id=\"fig10.3.2\"><\/a>Figure 10.3.2 image description:<\/strong> At 500 Ma, rocks in Europe had upward-pointing magnetic orientations. At 400 Ma, the magnetic orientation leveled. From 300 Ma to the present, rocks in Europe shown an increasingly downward-pointing magnetic orientation. <a href=\"#retfig10.3.2\">[Return to Figure 10.3.2]<\/a>\r\n\r\n<strong id=\"fig10.12\"><a id=\"fig10.3.6\"><\/a>Figure 10.3.6 image description:<\/strong> A cross section of the trench formed at the Aleutian subduction zone as the Pacific plate subducts under the North American plate in the middle of the Pacific Ocean. The farther away an earthquake is from this trench (on the North America plate side), the deeper it is. <a href=\"#retfig10.3.6\">[Return to Figure 10.3.6]<\/a>\r\n<h3>Media Attributions<\/h3>\r\n<ul>\r\n \t<li>Figures 10.3.1, 10.3.2, 10.3.3, 10.3.5, 10.3.6, 10.3.8, 10.3.11, 10.3.12, 10.3.13: \u00a9 Steven Earle. CC BY.<\/li>\r\n \t<li>Figure 10.3.4: \"<a href=\"https:\/\/commons.wikimedia.org\/wiki\/File:Elevation.jpg\">Elevation<\/a>\" by NOAA. Adapted by Steven Earle. Public domain.<\/li>\r\n \t<li>Figure 10.3.7: \"<a href=\"http:\/\/geomaps.wr.usgs.gov\/parks\/noca\/nocageol4c.html\">Juan de Fuca Ridge<\/a>\" by USGS. Adapted by Steven Earle. Public domain. Based on Raff, A. and Mason, R., 1961, Magnetic survey off the west coast of North America, 40\u02da N to 52\u02da N latitude, Geol. Soc. America Bulletin, V. 72, p. 267-270.<\/li>\r\n \t<li>Figure 10.3.9: \"<a href=\"http:\/\/en.wikipedia.org\/wiki\/Hotspot_(geology)#\/media\/File:Hawaii_hotspot.jpg\">Hawaii Hotspot<\/a>\" by <a href=\"https:\/\/www.ngdc.noaa.gov\/mgg\/image\/2minrelief.html\">National Geophysical Data Center<\/a>. Adapted by Steven Earle. Public domain.<\/li>\r\n \t<li>Figure 10.3.10: \"<a href=\"https:\/\/commons.wikimedia.org\/wiki\/File:Hotspots.jpg\">Hotspots<\/a>\" by\u00a0Ingo W\u00f6lbern. Public domain.<\/li>\r\n<\/ul>\r\n<\/div>","rendered":"<p>As the mineral magnetite (Fe<sub>3<\/sub>O<sub>4<\/sub>) crystallizes from magma, it becomes magnetized with an orientation parallel to that of Earth&#8217;s magnetic field at that time. This is called <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1617\">remnant magnetism<\/a><\/strong>. Rocks like basalt, which cool from a high temperature and commonly have relatively high levels of magnetite (up to 1 or 2%), are particularly susceptible to being magnetized in this way, but even sediments and sedimentary rocks, as long as they have small amounts of magnetite, will take on remnant magnetism because the magnetite grains gradually become reoriented following deposition. By studying both the horizontal and vertical components of the remnant magnetism, one can tell not only the direction to magnetic north at the time of the rock&#8217;s formation, but also the latitude where the rock formed relative to magnetic north.<\/p>\n<p>In the early 1950s, a group of geologists from Cambridge University, including Keith Runcorn, Ted Irving,<a class=\"footnote\" title=\"Ted Irving later set up a paleomagnetic lab at the Geological Survey of Canada in Sidney, B.C., and did a great deal of important work on understanding the geology of western North America.\" id=\"return-footnote-447-1\" href=\"#footnote-447-1\" aria-label=\"Footnote 1\"><sup class=\"footnote\">[1]<\/sup><\/a>\u00a0and several others, started looking at the remnant magnetism of Phanerozoic British and European volcanic rocks, and collecting <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1618\">paleomagnetic<\/a><\/strong> data. They found that rocks of different ages sampled from generally the same area showed quite different apparent magnetic pole positions (Figure 10.3.1). They initially assumed that this meant that Earth&#8217;s magnetic field had, over time, departed significantly from its present position\u2014which is close to the rotational pole.<\/p>\n<figure id=\"attachment_433\" aria-describedby=\"caption-attachment-433\" style=\"width: 700px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-433\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131.png\" alt=\"\" width=\"700\" height=\"348\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131.png 1061w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131-300x149.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131-768x381.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131-1024x509.png 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131-65x32.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131-225x112.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/06\/image0131-350x174.png 350w\" sizes=\"auto, (max-width: 700px) 100vw, 700px\" \/><\/a><figcaption id=\"caption-attachment-433\" class=\"wp-caption-text\">Figure 10.3.1 Apparent polar-wandering paths (APWP) for Eurasia and North America. The view is from the North Pole (black dot) looking down. The outer circle is the equator. In the diagram to the right the curve locations have been corrected taking continental drift into account.<\/figcaption><\/figure>\n<p>The curve defined by the paleomagnetic data was called a <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1619\">polar wandering path<\/a><\/strong> because Runcorn and his students initially thought that their data represented actual movement of the magnetic poles (since geophysical models of the time suggested that the magnetic poles did not need to be aligned with the rotational poles). We now know that the magnetic data define movement of continents, and <em>not<\/em> of the magnetic poles, so we call it an <em>apparent<\/em> polar wandering path (APWP).<\/p>\n<div class=\"textbox textbox--examples\">\n<header class=\"textbox__header\">\n<p class=\"textbox__title\">What is a polar wandering path?<a id=\"retfig10.3.2\"><\/a><\/p>\n<\/header>\n<div class=\"textbox__content\">\n<figure id=\"attachment_434\" aria-describedby=\"caption-attachment-434\" style=\"width: 400px\" class=\"wp-caption alignright\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0151.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-434\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0151.png\" alt=\"The magnetic orientation of rocks in Europe from 500 Ma to the present. Image description available\" width=\"400\" height=\"439\" \/><\/a><figcaption id=\"caption-attachment-434\" class=\"wp-caption-text\">Figure 10.3.2 <a href=\"#fig10.3.2\">[Image Description]<\/a><\/figcaption><\/figure>\n<p>At around 500 Ma, what we now call Europe was south of the equator, and so European rocks formed then would have acquired an upward-pointing magnetic field orientation (see Figure 9.3.2 and Figure 10.3.2). Between then and now, Europe gradually moved north, and the rocks forming at various times acquired steeper and steeper <em>downward-pointing<\/em> magnetic orientations.When researchers evaluated magnetic data in this way in the 1950s, they plotted where the North Pole would have appeared to be based on the magnetic data and assumed that the continent was always where it is now. That means that the 500 Ma \u201capparent\u201d north pole would have been somewhere in the South Pacific, and that over the following 500 million years it would have gradually moved north.Of course we now know that the magnetic poles don\u2019t move around much (although polarity reversals do take place) and that the reason Europe had a magnetic orientation characteristic of the southern hemisphere is that it was in the southern hemisphere at 500 Ma.Runcorn and colleagues soon extended their work to North America, and this also showed <em>apparent<\/em> polar wandering, but the results were not consistent with those from Europe. For example, the 200 Ma pole for North America plotted somewhere in China, while the 200 Ma pole for Europe plotted in the Pacific Ocean. Since there could only have been one pole position at 200 Ma, this evidence strongly supported the idea that North America and Europe had moved relative to each other since 200 Ma. Subsequent paleomagnetic work showed that South America, Africa, India, and Australia also have unique polar wandering curves. In 1956, Runcorn changed his mind and became a proponent of continental drift.This paleomagnetic work of the 1950s was the first new evidence in favour of continental drift, and it led a number of geologists to start thinking that the idea might have some merit. Nevertheless, for a majority of geologists working on global geology at the time, this type of evidence was not sufficiently convincing to get them to change their views.<\/div>\n<\/div>\n<p>During the 20th century, our knowledge and understanding of the ocean basins and their geology increased dramatically. Before 1900, we knew virtually nothing about the bathymetry and geology of the oceans. By the end of the 1960s, we had detailed maps of the topography of the ocean floors, a clear picture of the geology of ocean floor sediments and the solid rocks underneath them, and almost as much information about the geophysical nature of ocean rocks as of continental rocks.<\/p>\n<p>Up until about the 1920s, ocean depths were measured using weighted lines dropped overboard. In deep water this is a painfully slow process and the number of soundings in the deep oceans was probably fewer than 1,000. That is roughly one depth sounding for every 350,000 square kilometres of the ocean. To put that in perspective, it would be like trying to describe the topography of British Columbia with elevation data for only a half a dozen points! The voyage of the <em>Challenger<\/em> in 1872 and the laying of trans-Atlantic cables had shown that there were mountains beneath the seas, but most geologists and oceanographers still believed that the oceans were essentially vast basins with flat bottoms, filled with thousands of metres of sediments.<\/p>\n<p>Following development of acoustic depth sounders in the 1920s (Figure 10.3.3), the number of depth readings increased by many orders of magnitude, and by the 1930s, it had become apparent that there were major mountain chains in all of the world&#8217;s oceans. During and after World War II, there was a well-organized campaign to study the oceans, and by 1959, sufficient bathymetric data had been collected to produce detailed maps of all the oceans (Figure 10.3.4).<\/p>\n<figure id=\"attachment_435\" aria-describedby=\"caption-attachment-435\" style=\"width: 600px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0171.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-435\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0171.png\" alt=\"&quot;&quot;\" width=\"600\" height=\"267\" \/><\/a><figcaption id=\"caption-attachment-435\" class=\"wp-caption-text\">Figure 10.3.3 Depiction of a ship-borne acoustic depth sounder. The instrument emits a sound (black arcs) that bounces off the sea floor and returns to the surface (white arcs). The travel time is proportional to the water depth.<\/figcaption><\/figure>\n<figure id=\"attachment_436\" aria-describedby=\"caption-attachment-436\" style=\"width: 700px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-436\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4.jpg\" alt=\"\" width=\"700\" height=\"467\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4.jpg 2268w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4-300x200.jpg 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4-768x512.jpg 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4-1024x683.jpg 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4-65x43.jpg 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4-225x150.jpg 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/bathymetry-4-350x233.jpg 350w\" sizes=\"auto, (max-width: 700px) 100vw, 700px\" \/><\/a><figcaption id=\"caption-attachment-436\" class=\"wp-caption-text\">Figure 10.3.4 Ocean floor bathymetry (and continental topography). Inset (a): the mid-Atlantic ridge, (b): the Newfoundland continental shelf, (c): the Nazca trench adjacent to South America, and (d): the Hawaiian Island chain.<\/figcaption><\/figure>\n<p>The important physical features of the ocean floor are:<\/p>\n<ul>\n<li>Extensive linear ridges (commonly in the central parts of the oceans) with water depths in the order of 2,000 to 3,000 m (Figure 10.3.4, inset a)<\/li>\n<li>Fracture zones perpendicular to the ridges (inset a)<\/li>\n<li>Deep-ocean plains at depths of 5,000 to 6,000 m (insets a and d)<\/li>\n<li>Relatively flat and shallow continental shelves with depths under 500 m (inset b)<\/li>\n<li>Deep trenches (up to 11,000 m deep), most near the continents (inset c)<\/li>\n<li>Seamounts and chains of seamounts (inset d)<\/li>\n<\/ul>\n<p><strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1620\">Seismic reflection sounding<\/a><\/strong> involves transmitting high-energy sound bursts and then measuring the echos with a series of geophones towed behind a ship. The technique is related to <em>acoustic sounding<\/em> as described above; however, much more energy is transmitted and the sophistication of the data processing is much greater. As the technique evolved, and the amount of energy was increased, it became possible to <em>see through<\/em> the sea-floor sediments and map the bedrock topography and crustal thickness. Hence sediment thicknesses could be mapped, and it was soon discovered that although the sediments were up to several thousands of metres thick near the continents, they were relatively thin \u2014 or even non-existent \u2014 in the ocean ridge areas (Figure 10.3.5). The seismic studies also showed that the crust is relatively thin under the oceans (5 km to 6 km) compared to the continents (30 km to 60 km) and geologically very consistent, composed almost entirely of basalt.<\/p>\n<figure id=\"attachment_437\" aria-describedby=\"caption-attachment-437\" style=\"width: 800px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-437\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments.png\" alt=\"\" width=\"800\" height=\"163\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments.png 1219w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments-300x61.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments-768x156.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments-1024x208.png 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments-65x13.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments-225x46.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/sediments-350x71.png 350w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><\/a><figcaption id=\"caption-attachment-437\" class=\"wp-caption-text\">Figure 10.3.5 Topographic section at an ocean ridge based on reflection seismic data. Sediments are not thick enough to be detectable near the ridge, but get thicker on either side. The diagram represents approximately 50 km width, and has a 10x vertical exaggeration.<\/figcaption><\/figure>\n<p>In the early 1950s, Edward Bullard, who spent time at the University of Toronto but is mostly associated with Cambridge University, developed a probe for measuring the flow of heat from the ocean floor. Bullard and colleagues found the rate to be higher than average along the ridges, and lower than average in the trench areas. Although Bullard was a plate-tectonics sceptic, these features were interpreted to indicate that there is convection within the mantle \u2014 the areas of high heat flow being correlated with upward convection of hot mantle material, and the areas of low heat flow being correlated with downward convection.<\/p>\n<p>With developments of networks of seismographic stations in the 1950s, it became possible to plot the locations <em>and<\/em> depths of both major and minor earthquakes with great accuracy. It was found that there is a remarkable correspondence between earthquakes and both the mid-ocean ridges and the deep ocean trenches. In 1954 Gutenberg and Richter showed that the ocean-ridge earthquakes were all relatively shallow, and confirmed what had first been shown by Benioff in the 1930s \u2014 that earthquakes in the vicinity of ocean trenches were both shallow and deep, but that the deeper ones were situated progressively farther inland from the trenches (Figure 10.3.6).<a id=\"retfig10.3.6\"><\/a><\/p>\n<figure id=\"attachment_438\" aria-describedby=\"caption-attachment-438\" style=\"width: 800px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-438\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes.png\" alt=\"\" width=\"800\" height=\"182\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes.png 1248w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes-300x68.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes-768x175.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes-1024x233.png 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes-65x15.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes-225x51.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/trench-quakes-350x80.png 350w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><\/a><figcaption id=\"caption-attachment-438\" class=\"wp-caption-text\">Figure 10.3.6 Cross-section through the Aleutian subduction zone with a depiction of the increasing depth of earthquakes \u201cinshore\u201d from the trench. <a href=\"#fig10.3.6\">[Image Description]<\/a><\/figcaption><\/figure>\n<p>In the 1950s, scientists from the Scripps Oceanographic Institute in California persuaded the U.S. Coast Guard to include magnetometer readings on one of their expeditions to study ocean floor topography. The first comprehensive magnetic data set was compiled in 1958 for an area off the coast of B.C. and Washington State. This survey revealed a bewildering pattern of low and high magnetic intensity in sea-floor rocks (Figure 10.3.7). When the data were first plotted on a map in 1961, nobody understood them \u2014 not even the scientists who collected them. Although the patterns made even less sense than the stripes on a zebra, many thousands of kilometres of magnetic surveys were conducted over the next several years.<\/p>\n<figure id=\"attachment_439\" aria-describedby=\"caption-attachment-439\" style=\"width: 350px\" class=\"wp-caption alignright\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-439\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason.png\" alt=\"\" width=\"350\" height=\"282\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason.png 497w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason-300x241.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason-65x52.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason-225x181.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/raff-mason-350x282.png 350w\" sizes=\"auto, (max-width: 350px) 100vw, 350px\" \/><\/a><figcaption id=\"caption-attachment-439\" class=\"wp-caption-text\">Figure 10.3.7 Pattern of sea-floor magnetism off of the west coast of British Columbia and Washington.<\/figcaption><\/figure>\n<p>The wealth of new data from the oceans began to significantly influence geological thinking in the 1960s. In 1960, Harold Hess, a widely respected geologist from Princeton University, advanced a theory with many of the elements that we now accept as <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1356\">plate tectonics<\/a><\/strong>. He maintained some uncertainty about his proposal however, and in order to deflect criticism from mainstream geologists, he labelled it <em>geopoetry<\/em>. In fact, until 1962, Hess didn&#8217;t even put his ideas in writing\u2014except internally to the U.S. Navy (which funded his research)\u2014but presented them mostly in lectures and seminars. Hess proposed that new sea floor was generated from mantle material at the ocean ridges, and that old sea floor was dragged down at the ocean trenches and re-incorporated into the mantle. He suggested that the process was driven by mantle convection currents, rising at the ridges and descending at the trenches (Figure 10.3.8). He also suggested that the less-dense continental crust did not descend with oceanic crust into trenches, but that colliding land masses were thrust up to form mountains. Hess&#8217;s theory formed the basis for our ideas on <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1621\">sea-floor spreading<\/a><\/strong> and <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1622\">continental drift<\/a><\/strong><strong>,<\/strong> but it did not deal with the concept that the crust is made up of specific <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1624\">plates<\/a><\/strong>. Although the Hess model was not roundly criticized, it was not widely accepted (especially in the U.S.), partly because it was not well supported by hard evidence.<\/p>\n<figure id=\"attachment_440\" aria-describedby=\"caption-attachment-440\" style=\"width: 800px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-440\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model.png\" alt=\"\" width=\"800\" height=\"265\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model.png 1091w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model-300x100.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model-768x255.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model-1024x340.png 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model-65x22.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model-225x75.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hess-model-350x116.png 350w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><\/a><figcaption id=\"caption-attachment-440\" class=\"wp-caption-text\">Figure 10.3.8 A representation of Harold Hess\u2019s model for sea-floor spreading and subduction.<\/figcaption><\/figure>\n<p>Collection of magnetic data from the oceans continued in the early 1960s, but still nobody could explain the origin of the zebra-like patterns. Most assumed that they were related to variations in the composition of the rocks\u2014such as variations in the amount of magnetite\u2014as this is a common explanation for magnetic variations in rocks of the continental crust. The first real understanding of the significance of the striped anomalies was the interpretation by Fred Vine, a Cambridge graduate student. Vine was examining magnetic data from the Indian Ocean and, like others before, he noted the symmetry of the magnetic patterns with respect to the oceanic ridge.<\/p>\n<p>At the same time, other researchers, led by groups in California and New Zealand, were studying the phenomenon of reversals in Earth&#8217;s magnetic field. They were trying to determine when such reversals had taken place over the past several million years by analyzing the magnetic characteristics of hundreds of samples from basaltic flows. As discussed in Chapter 9, it is evident that Earth\u2019s magnetic field becomes weakened periodically and then virtually non-existent, before becoming re-established with the reverse polarity. During periods of reversed polarity, a compass would point south instead of north.<\/p>\n<p>The time scale of magnetic reversals is irregular. For example, the present &#8220;normal&#8221; event, known as the Bruhnes magnetic chron, has persisted for about 780,000 years. This was preceded by a 190,000-year reversed event; a 50,000-year normal event known as Jaramillo; and then a 700,000-year reversed event (see Figure 9.3.3).<\/p>\n<p>In a paper published in September 1963, Vine and his PhD supervisor Drummond Matthews proposed that the patterns associated with ridges were related to the magnetic reversals, and that oceanic crust created from cooling basalt during a <em>normal<\/em> event would have polarity aligned with the present magnetic field, and thus would produce a positive anomaly (a black stripe on the sea-floor magnetic map), whereas oceanic crust created during a <em>reversed<\/em> event would have polarity opposite to the present field and thus would produce a negative magnetic anomaly (a white stripe). The same idea had been put forward a few months earlier by Lawrence Morley, of the Geological Survey of Canada; however, his papers submitted earlier in 1963 to <em>Nature<\/em> and <em>The Journal of Geophysical Research<\/em> were rejected. Many people refer to the idea as the Vine-Matthews-Morley (VMM) hypothesis.<\/p>\n<p>Vine, Matthews, and Morley were the first to show this type of correspondence between the relative widths of the stripes and the periods of the magnetic reversals. The VMM hypothesis was confirmed within a few years when magnetic data were compiled from spreading ridges around the world. It was shown that the same general magnetic patterns were present straddling each ridge, although the widths of the anomalies varied according to the spreading rates characteristic of the different ridges. It was also shown that the patterns corresponded with the chronology of Earth&#8217;s magnetic field reversals. This global consistency provided strong support for the VMM hypothesis and led to rejection of the other explanations for the magnetic anomalies.<\/p>\n<p>In 1963, J. Tuzo Wilson of the University of Toronto proposed the idea of a <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1160\">mantle plume<\/a><\/strong> or <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1625\">hot spot<\/a><\/strong>\u2014a place where hot mantle material rises in a stationary and semi-permanent plume, and affects the overlying crust. He based this hypothesis partly on the distribution of the Hawaiian and Emperor Seamount island chains in the Pacific Ocean (Figure 10.3.9). The volcanic rock making up these islands gets progressively younger toward the southeast, culminating with the island of Hawaii itself, which consists of rock that is almost all younger than 1 Ma. Wilson suggested that a stationary plume of hot upwelling mantle material is the source of the Hawaiian volcanism, and that the ocean crust of the Pacific Plate is moving toward the northwest over this hot spot. Near the Midway Islands, the chain takes a pronounced change in direction, from northwest-southeast for the Hawaiian Islands and to nearly north-south for the Emperor Seamounts. This change is widely ascribed to a change in direction of the Pacific Plate moving over the stationary mantle plume, but a more plausible explanation is that the Hawaiian mantle plume has not actually been stationary throughout its history, and in fact moved at least 2,000 km south over the period between 81 and 45 Ma.<a class=\"footnote\" title=\"J. A. Tarduno et al., 2003, The Emperor Seamounts: Southward Motion of the Hawaiian Hotspot Plume in Earth\u2019s Mantle,\u00a0Science\u00a0301\u00a0(5636): 1064\u20131069.\" id=\"return-footnote-447-2\" href=\"#footnote-447-2\" aria-label=\"Footnote 2\"><sup class=\"footnote\">[2]<\/sup><\/a><\/p>\n<figure id=\"attachment_441\" aria-describedby=\"caption-attachment-441\" style=\"width: 784px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-441 size-full\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312.png\" alt=\"\" width=\"784\" height=\"573\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312.png 784w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312-300x219.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312-768x561.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312-65x48.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312-225x164.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0312-350x256.png 350w\" sizes=\"auto, (max-width: 784px) 100vw, 784px\" \/><\/a><figcaption id=\"caption-attachment-441\" class=\"wp-caption-text\">Figure 10.3.9 The ages of the Hawaiian Islands and the Emperor Seamounts in relation to the location of the Hawaiian mantle plume.<\/figcaption><\/figure>\n<div class=\"textbox textbox--exercises\">\n<header class=\"textbox__header\">\n<p class=\"textbox__title\">Exercise 10.2 Volcanoes and the Rate of Plate Motion<\/p>\n<\/header>\n<div class=\"textbox__content\">\n<p>The Hawaiian and Emperor volcanoes shown in Figure 10.3.9 are listed in the table below along with their ages and their distances from the centre of the mantle plume under Hawaii (the Big Island).<\/p>\n<table>\n<caption>Ages of Hawaiian and Emperor volcanoes and their distances from the centre of the mantle plume. Calculate their rate of movement in centimetres per year.\u00a0<\/caption>\n<tbody>\n<tr>\n<th scope=\"col\">Island<\/th>\n<th scope=\"col\">Age<\/th>\n<th scope=\"col\">Distance<\/th>\n<th scope=\"col\">Rate<\/th>\n<\/tr>\n<tr>\n<td>Hawaii<\/td>\n<td>0 Ma<\/td>\n<td>0 km<\/td>\n<td>&#8211;<\/td>\n<\/tr>\n<tr>\n<td>Necker<\/td>\n<td>10.3 Ma<\/td>\n<td>1,058 km<\/td>\n<td>10.2 cm\/y<\/td>\n<\/tr>\n<tr>\n<td>Midway<\/td>\n<td>27.7 Ma<\/td>\n<td>2,432 km<\/td>\n<td><\/td>\n<\/tr>\n<tr>\n<td>Koko<\/td>\n<td>48.1 Ma<\/td>\n<td>3,758 km<\/td>\n<td><\/td>\n<\/tr>\n<tr>\n<td>Suiko<\/td>\n<td>64.7 Ma<\/td>\n<td>4,860 km<\/td>\n<td><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>Plot the data on the graph provided here, and use the numbers in the table to estimate the rates of plate motion for the Pacific Plate in cm\/year. (The first two are plotted for you.)<\/p>\n<p><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0331.png\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-442\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0331.png\" alt=\"A blank graph. Distance (in kilometres) on y-axis. Age (Ma) on x-axis\" width=\"600\" height=\"403\" \/><\/a><\/p>\n<p>See Appendix 3 for <a href=\"\/physicalgeology2ed\/back-matter\/appendix-3-answers-to-exercises\/#exercisea10.2\">Exercise 10.2 answers<\/a>.<\/p>\n<\/div>\n<\/div>\n<p>There is evidence of many such mantle plumes around the world (Figure 10.3.10). Most are within the ocean basins\u2014including places like Hawaii, Iceland, and the Galapagos Islands\u2014but some are under continents. One example is the Yellowstone hot spot in the west-central United States, and another is the one responsible for the Anahim Volcanic Belt in central British Columbia. It is evident that mantle plumes are very long-lived phenomena, lasting for at least tens of millions of years, possibly for hundreds of millions of years in some cases.<\/p>\n<figure id=\"attachment_443\" aria-describedby=\"caption-attachment-443\" style=\"width: 884px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-443 size-full\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots.png\" alt=\"\" width=\"884\" height=\"514\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots.png 884w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots-300x174.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots-768x447.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots-65x38.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots-225x131.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/hot-spots-350x204.png 350w\" sizes=\"auto, (max-width: 884px) 100vw, 884px\" \/><\/a><figcaption id=\"caption-attachment-443\" class=\"wp-caption-text\">Figure 10.3.10 Mantle plume locations. Selected Mantle plumes: 1: Azores, 3: Bowie, 5: Cobb, 8: Eifel, 10: Galapagos, 12: Hawaii, 14: Iceland, 17: Cameroon, 18: Canary, 19: Cape Verde, 35: Samoa, 38: Tahiti, 42: Tristan, 44: Yellowstone, 45: Anahim<\/figcaption><\/figure>\n<p>Although oceanic spreading ridges appear to be curved features on Earth&#8217;s surface, in fact the ridges are composed of a series of straight-line segments, offset at intervals by faults perpendicular to the ridge (Figure 10.3.11). In a paper published in 1965, Tuzo Wilson termed these features <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1626\">transform faults<\/a><\/strong>. He described the nature of the motion along them, and showed why there are earthquakes only on the section of a transform fault between two adjacent ridge segments. The San Andreas Fault in California is a very long transform fault that links the southern end of the Juan de Fuca spreading ridge to the East Pacific Rise spreading ridges situated in the Gulf of California (see Figure 10.4.9). The Queen Charlotte Fault, which extends north from the northern end of the Juan de Fuca spreading ridge (near the northern end of Vancouver Island) toward Alaska, is also a transform fault.<\/p>\n<figure id=\"attachment_444\" aria-describedby=\"caption-attachment-444\" style=\"width: 800px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-444\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform.png\" alt=\"\" width=\"800\" height=\"316\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform.png 1085w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-300x118.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-768x303.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-1024x404.png 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-65x26.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-225x89.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-350x138.png 350w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><\/a><figcaption id=\"caption-attachment-444\" class=\"wp-caption-text\">Figure 10.3.11 A part of the mid-Atlantic ridge near the equator. The double white lines are spreading ridges. The solid white lines are fracture zones. As shown by the yellow arrows, the relative motion of the plates on either side of the fracture zones can be similar (arrows pointing the same direction) or opposite (arrows pointing opposite directions). Transform faults (red lines) are in between the ridge segments, where the yellow arrows point in opposite directions.<\/figcaption><\/figure>\n<p>In the same 1965 paper, Wilson introduced the idea that the crust can be divided into a series of rigid plates, and thus he is responsible for the term <strong><a class=\"glossary-term\" aria-haspopup=\"dialog\" aria-describedby=\"definition\" href=\"#term_447_1356\">plate tectonics<\/a><\/strong>.<\/p>\n<div class=\"textbox textbox--exercises\">\n<header class=\"textbox__header\">\n<p class=\"textbox__title\">Exercise 10.3 Paper transform fault model<\/p>\n<\/header>\n<div class=\"textbox__content\">\n<figure id=\"attachment_445\" aria-describedby=\"caption-attachment-445\" style=\"width: 950px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-445\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model.png\" alt=\"\" width=\"950\" height=\"379\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model.png 1153w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model-300x120.png 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model-768x306.png 768w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model-1024x409.png 1024w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model-65x26.png 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model-225x90.png 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/transform-model-350x140.png 350w\" sizes=\"auto, (max-width: 950px) 100vw, 950px\" \/><\/a><figcaption id=\"caption-attachment-445\" class=\"wp-caption-text\">Figure 10.3.12<\/figcaption><\/figure>\n<p>Tuzo Wilson used a paper model, a little bit like the one shown here, to explain transform faults to his colleagues. To use this model either print this page or download the image above and print that, then cut around the outside, and then slice along the line A-B (the fracture zone) with a sharp knife. Fold down the top half where shown, and then pinch together in the middle. Do the same with the bottom half.<\/p>\n<figure id=\"attachment_446\" aria-describedby=\"caption-attachment-446\" style=\"width: 400px\" class=\"wp-caption alignright\"><a href=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-446 size-full\" src=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411.jpg\" alt=\"\" width=\"400\" height=\"266\" srcset=\"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411.jpg 400w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411-300x200.jpg 300w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411-65x43.jpg 65w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411-225x150.jpg 225w, https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-content\/uploads\/sites\/298\/2019\/08\/image0411-350x233.jpg 350w\" sizes=\"auto, (max-width: 400px) 100vw, 400px\" \/><\/a><figcaption id=\"caption-attachment-446\" class=\"wp-caption-text\">Figure 10.3.13<\/figcaption><\/figure>\n<p>When you\u2019re done, you should have something like the example shown on Figure 10.3.13, with two folds of paper extending underneath. Find someone else to pinch those folds with two fingers just below each ridge crest, and then gently pull apart where shown. As you do, the oceanic crust will emerge from the middle, and you\u2019ll see that the parts of the fracture zone between the ridge crests will be moving in opposite directions (this is the transform fault) while the parts of the fracture zone outside of the ridge crests will be moving in the same direction. You\u2019ll also see that the oceanic crust is being magnetized as it forms at the ridge. The magnetic patterns shown are accurate, and represent the last 2.5 Ma of geological time.<\/p>\n<p>There are other versions of this model available here: <a href=\"https:\/\/web.viu.ca\/earle\/transform-model\/\">Paper Models of Transform Faults<\/a>.<a class=\"footnote\" title=\"For more information see: Earle, S., 2004,\u00a0A simple paper model of a transform fault at a spreading ridge,\u00a0J. Geosc. Educ.\u00a0V. 52, p. 391-2.\" id=\"return-footnote-447-3\" href=\"#footnote-447-3\" aria-label=\"Footnote 3\"><sup class=\"footnote\">[3]<\/sup><\/a><\/p>\n<p>See Appendix 3 for <a href=\"\/physicalgeology2ed\/back-matter\/appendix-3-answers-to-exercises\/#exercisea10.3\">Exercise 10.3 answers<\/a>.<\/p>\n<\/div>\n<\/div>\n<div>\n<h3>Image Descriptions<\/h3>\n<p><strong id=\"fig10.8\"><a id=\"fig10.3.2\"><\/a>Figure 10.3.2 image description:<\/strong> At 500 Ma, rocks in Europe had upward-pointing magnetic orientations. At 400 Ma, the magnetic orientation leveled. From 300 Ma to the present, rocks in Europe shown an increasingly downward-pointing magnetic orientation. <a href=\"#retfig10.3.2\">[Return to Figure 10.3.2]<\/a><\/p>\n<p><strong id=\"fig10.12\"><a id=\"fig10.3.6\"><\/a>Figure 10.3.6 image description:<\/strong> A cross section of the trench formed at the Aleutian subduction zone as the Pacific plate subducts under the North American plate in the middle of the Pacific Ocean. The farther away an earthquake is from this trench (on the North America plate side), the deeper it is. <a href=\"#retfig10.3.6\">[Return to Figure 10.3.6]<\/a><\/p>\n<h3>Media Attributions<\/h3>\n<ul>\n<li>Figures 10.3.1, 10.3.2, 10.3.3, 10.3.5, 10.3.6, 10.3.8, 10.3.11, 10.3.12, 10.3.13: \u00a9 Steven Earle. CC BY.<\/li>\n<li>Figure 10.3.4: &#8220;<a href=\"https:\/\/commons.wikimedia.org\/wiki\/File:Elevation.jpg\">Elevation<\/a>&#8221; by NOAA. Adapted by Steven Earle. Public domain.<\/li>\n<li>Figure 10.3.7: &#8220;<a href=\"http:\/\/geomaps.wr.usgs.gov\/parks\/noca\/nocageol4c.html\">Juan de Fuca Ridge<\/a>&#8221; by USGS. Adapted by Steven Earle. Public domain. Based on Raff, A. and Mason, R., 1961, Magnetic survey off the west coast of North America, 40\u02da N to 52\u02da N latitude, Geol. Soc. America Bulletin, V. 72, p. 267-270.<\/li>\n<li>Figure 10.3.9: &#8220;<a href=\"http:\/\/en.wikipedia.org\/wiki\/Hotspot_(geology)#\/media\/File:Hawaii_hotspot.jpg\">Hawaii Hotspot<\/a>&#8221; by <a href=\"https:\/\/www.ngdc.noaa.gov\/mgg\/image\/2minrelief.html\">National Geophysical Data Center<\/a>. Adapted by Steven Earle. Public domain.<\/li>\n<li>Figure 10.3.10: &#8220;<a href=\"https:\/\/commons.wikimedia.org\/wiki\/File:Hotspots.jpg\">Hotspots<\/a>&#8221; by\u00a0Ingo W\u00f6lbern. Public domain.<\/li>\n<\/ul>\n<\/div>\n<hr class=\"before-footnotes clear\" \/><div class=\"footnotes\"><ol><li id=\"footnote-447-1\">Ted Irving later set up a paleomagnetic lab at the Geological Survey of Canada in Sidney, B.C., and did a great deal of important work on understanding the geology of western North America. <a href=\"#return-footnote-447-1\" class=\"return-footnote\" aria-label=\"Return to footnote 1\">&crarr;<\/a><\/li><li id=\"footnote-447-2\">J. A. Tarduno et al., 2003, The Emperor Seamounts: Southward Motion of the Hawaiian Hotspot Plume in Earth\u2019s Mantle,\u00a0Science\u00a0301\u00a0(5636): 1064\u20131069. <a href=\"#return-footnote-447-2\" class=\"return-footnote\" aria-label=\"Return to footnote 2\">&crarr;<\/a><\/li><li id=\"footnote-447-3\">For more information see: Earle, S., 2004,\u00a0<em>A simple paper model of a transform fault at a spreading ridge<\/em>,\u00a0J. Geosc. Educ.\u00a0V. 52, p. 391-2. <a href=\"#return-footnote-447-3\" class=\"return-footnote\" aria-label=\"Return to footnote 3\">&crarr;<\/a><\/li><\/ol><\/div><div class=\"glossary\"><span class=\"screen-reader-text\" id=\"definition\">definition<\/span><template id=\"term_447_1617\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1617\"><div tabindex=\"-1\"><p>magnetism of a body of rock that formed at the time the rock formed and is consistent with the magnetic field orientation that existed at that time and place<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1618\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1618\"><div tabindex=\"-1\"><p>past variations in the intensity and polarity of the Earth\u2019s magnetic field<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1619\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1619\"><div tabindex=\"-1\"><p>a path of varying magnetic pole positions defined by paleomagnetic data (in fact it is now understood that the continents have wandered, not the poles, so a more appropriate terms is \u201capparent polar wandering path\u201d)<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1620\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1620\"><div tabindex=\"-1\"><p>measurement of the properties of sediments based on detection of sounds generated at surface and reflected from layers beneath the surface<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1356\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1356\"><div tabindex=\"-1\"><p>The concept that the Earth\u2019s crust and upper mantle (lithosphere) is divided into a number of plates that move independently on the surface and interact with each other at their boundaries.<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1621\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1621\"><div tabindex=\"-1\"><p>the formation of new oceanic crust by volcanism at a divergent plate boundary<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1622\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1622\"><div tabindex=\"-1\"><p>the concept that tectonic plates can move across the surface of the Earth<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1624\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1624\"><div tabindex=\"-1\"><p>a region of the lithosphere that is considered to be moving across the surface of the Earth as a single unit<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1160\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1160\"><div tabindex=\"-1\"><p>a plume of hot rock (not magma) that rises through the mantle (either from the base or from part way up) and reaches the surface where it spreads out and also leads to hot-spot volcanism<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1625\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1625\"><div tabindex=\"-1\"><p>the surface area of volcanism and high heat flow above a mantle plume<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><template id=\"term_447_1626\"><div class=\"glossary__definition\" role=\"dialog\" data-id=\"term_447_1626\"><div tabindex=\"-1\"><p>a boundary between two plates that are moving horizontally with respect to each other<\/p>\n<\/div><button><span aria-hidden=\"true\">&times;<\/span><span class=\"screen-reader-text\">Close definition<\/span><\/button><\/div><\/template><\/div>","protected":false},"author":90,"menu_order":3,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":"cc-by"},"chapter-type":[],"contributor":[],"license":[52],"class_list":["post-447","chapter","type-chapter","status-publish","hentry","license-cc-by"],"part":421,"_links":{"self":[{"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/chapters\/447","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/wp\/v2\/users\/90"}],"version-history":[{"count":4,"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/chapters\/447\/revisions"}],"predecessor-version":[{"id":2319,"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/chapters\/447\/revisions\/2319"}],"part":[{"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/parts\/421"}],"metadata":[{"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/chapters\/447\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/wp\/v2\/media?parent=447"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/pressbooks\/v2\/chapter-type?post=447"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/wp\/v2\/contributor?post=447"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/opentextbc.ca\/physicalgeology2ed\/wp-json\/wp\/v2\/license?post=447"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}