{"id":106,"date":"2021-09-16T19:28:33","date_gmt":"2021-09-16T19:28:33","guid":{"rendered":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/chapter\/3-2-magma-and-magma-formation-physical-geology-2nd-edition\/"},"modified":"2021-09-16T19:42:59","modified_gmt":"2021-09-16T19:42:59","slug":"3-2-magma-and-magma-formation-physical-geology-2nd-edition","status":"publish","type":"chapter","link":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/chapter\/3-2-magma-and-magma-formation-physical-geology-2nd-edition\/","title":{"raw":"3.2 Magma and Magma Formation -- Physical Geology &#8211; 2nd Edition","rendered":"3.2 Magma and Magma Formation &#8212; Physical Geology &#8211; 2nd Edition"},"content":{"raw":"\n\n<div><div>\n    <img src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/earths-crust2.png\" alt=\"Elements in the Earth's crust. Long decriptions available\" class=\"wp-image-118\" width=\"700\" height=\"484\">\n    <div class=\"wp-caption-text\" id=\"caption-attachment-121\">Figure 3.2.1 Average elemental proportions in Earth\u2019s crust, which is close to the average composition of magmas within the crust. <a href=\"#fig3.2.1\">[Image Description]<\/a><\/div>\n  <\/div>\n  <p>Virtually all of the igneous rocks that we see on Earth are derived from magmas that formed from <strong><span class=\"glossary-term\">partial melting<\/span><\/strong> of existing rock, either in the upper mantle or the crust. Partial melting is what happens when only some parts of a rock melt; it takes place because rocks are not pure materials. Most rocks are made up of several minerals, each of which has a different melting temperature. The wax in a candle is a pure material. If you put some wax into a warm oven (50\u00b0C will do as the melting temperature of most wax is about 40\u00b0C) and leave it there for a while, it will soon start to melt. That\u2019s complete melting, not partial melting. If instead you took a mixture of wax, plastic, aluminum, and glass and put it into the same warm oven, the wax would soon start to melt, but the plastic, aluminum, and glass would not melt (Figure 3.2.2a). That\u2019s partial melting and the result would be solid plastic, aluminum, and glass surrounded by liquid wax (Figure 3.2.2b). If we heat the oven up to around 120\u00b0C, the plastic would melt too and mix with the liquid wax, but the aluminum and glass would remain solid (Figure 3.2.2c). Again this is partial melting. If we separated the wax\/plastic \u201cmagma\u201d from the other components and let it cool, it would eventually harden. As you can see from Figure 3.2.2d, the liquid wax and plastic have mixed, and on cooling, have formed what looks like a single solid substance. It is most likely that this is a very fine-grained mixture of solid wax and solid plastic, but it could also be some other substance that has formed from the combination of the two.<\/p>\n  <div class=\"wp-caption aligncenter\" style=\"width: 700px\">\n    <img src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/pretend-rock-1024x1003-1.png\" alt=\"\" class=\"wp-image-119\" width=\"700\" height=\"686\">\n    <div class=\"wp-caption-text\">Figure 3.2.2 Partial melting of \u201cpretend rock\u201d: (a) the original components of white candle wax, black plastic pipe, green beach glass, and aluminum wire, (b) after heating to 50\u02daC for 30 minutes only the wax has melted, (c) after heating to 120\u02daC for 60 minutes much of the plastic has melted and the two liquids have mixed, (d) the liquid has been separated from the solids and allowed to cool to make a \u201cpretend rock\u201d with a different overall composition.<\/div>\n  <\/div>\n  <p>In this example, we partially melted some pretend rock to create some pretend magma. We then separated the magma from the source and allowed it to cool to make a new pretend rock with a composition quite different from the original material (it lacks glass and aluminum).<\/p>\n  <p>Of course partial melting in the real world isn\u2019t exactly the same as in our pretend-rock example. The main differences are that rocks are much more complex than the four-component system we used, and the mineral components of most rocks have more similar melting temperatures, so two or more minerals are likely to melt at the same time to varying degrees. Another important difference is that when rocks melt, the process takes thousands to millions of years, not the 90 minutes it took in the pretend-rock example.<\/p>\n  <p>Contrary to what one might expect, and contrary to what we did to make our pretend rock, most partial melting of real rock does not involve heating the rock up. The two main mechanisms through which rocks melt are <strong><span class=\"glossary-term\">decompression melting<\/span><\/strong> and <strong><span class=\"glossary-term\">flux melting<\/span><\/strong>. Decompression melting takes place within Earth when a body of rock is held at approximately the same temperature but the pressure is reduced. This happens because the rock is being moved toward the surface, either at a <strong><span class=\"glossary-term\">mantle plume<\/span><\/strong> (a.k.a., hot spot), or in the upwelling part of a mantle convection cell.<a class=\"footnote\" title=\"Mantle plumes are described in Chapter 4 and mantle convection in Chapter 9.\" id=\"return-footnote-123-1\" href=\"#footnote-123-1\"><sup class=\"footnote\">[1]<\/sup><\/a>&nbsp;The mechanism of decompression melting is shown in Figure 3.2.3a. If a rock that is hot enough to be close to its melting point is moved toward the surface, the pressure is reduced, and the rock can pass to the liquid side of its melting curve. At this point, <em>partial<\/em> melting starts to take place. The process of flux melting is shown in Figure 3.2.3b. If a rock is close to its melting point and some water (a flux that promotes melting) is added to the rock, the melting temperature is reduced (solid line versus dotted line), and partial melting starts.<a id=\"retfig3.2.3\" href=\"\"><\/a><\/p>\n  <div class=\"wp-caption aligncenter\" style=\"width: 700px\">\n    <img src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/flux-decompression.png\" alt=\"Graphs describing the melting curve for dry and wet mantle rock. Long description available\" class=\"wp-image-120\" width=\"700\" height=\"317\">\n    <div class=\"wp-caption-text\">Figure 3.2.3 Mechanisms for (a) decompression melting (the rock is moved toward the surface) and (b) flux melting (water is added to the rock) and the melting curve is displaced. <a href=\"#fig3.2.3\">[Image Description]<\/a><\/div>\n  <\/div>\n  <p>The partial melting of rock happens in a wide range of situations, most of which are related to plate tectonics. The more important of these are shown in Figure 3.2.3. At both mantle plumes and in the upward parts of convection systems, rock is being moved toward the surface, the pressure is dropping, and at some point, the rock crosses to the liquid side of its melting curve. At subduction zones, water from the wet, subducting oceanic crust is transferred into the overlying hot mantle. This provides the flux needed to lower the melting temperature. In both of these cases, only partial melting takes place\u2014typically only about 10% of the rock melts\u2014and it is always the most silica-rich components of the rock that melt, creating a magma that is more silica-rich than the rock from which it is derived. (By analogy, the melt from our pretend rock is richer in wax and plastic than the \u201crock\u201d from which it was derived.) The magma produced, being less dense than the surrounding rock, moves up through the mantle, and eventually into the crust.<\/p>\n  <div class=\"wp-caption aligncenter\" style=\"width: 850px\">\n    <img src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/magma-formation2-1024x447-1.png\" alt=\"\" class=\"wp-image-121\" width=\"850\" height=\"371\">\n    <div class=\"wp-caption-text\">Figure 3.2.4 Common sites of magma formation in the upper mantle. The black circles are regions of partial melting. The blue arrows represent water being transferred from the subducting plates into the overlying mantle.<\/div>\n  <\/div>\n  <p>As it moves toward the surface, and especially when it moves from the mantle into the lower crust, the hot magma interacts with the surrounding rock. This typically leads to partial melting of the surrounding rock because most such magmas are hotter than the melting temperature of crustal rock. (In this case, melting is caused by an increase in temperature.) Again, the more silica-rich parts of the surrounding rock are preferentially melted, and this contributes to an increase in the silica content of the magma.<\/p>\n  <p>At very high temperatures (over 1300\u00b0C), most magma is entirely liquid because there is too much energy for the atoms to bond together. As the temperature drops, usually because the magma is slowly moving upward, things start to change. Silicon and oxygen combine to form silica tetrahedra, and then, as cooling continues, the tetrahedra start to link together to make chains (<strong><span class=\"glossary-term\">polymerize<\/span><\/strong>). These silica chains have the important effect of making the magma more viscous (less runny), and as we\u2019ll see in Chapter 4, magma viscosity has significant implications for volcanic eruptions. As the magma continues to cool, crystals start to form.<\/p>\n  <div class=\"textbox textbox--exercises\">\n    <div class=\"textbox__header\">\n      <p>This is an experiment that you can do at home to help you understand the properties of magma. It will only take about 15 minutes, and all you need is half a cup of water and a few tablespoons of flour.<\/p>\n      <p>If you\u2019ve ever made gravy, white sauce, or roux, you\u2019ll know how this works.<\/p>\n      <p>Place about 1\/2 cup (125 mL) of water in a saucepan over medium heat. Add 2 teaspoons (10 mL) of white flour (this represents silica) and stir while the mixture comes close to boiling. It should thicken like gravy because the gluten in the flour becomes polymerized into chains during this process.<\/p>\n      <p>Now you\u2019re going to add more \u201csilica\u201d to see how this changes the viscosity of your magma. Take another 4 teaspoons (20 mL) of flour&nbsp;and mix it thoroughly with about 4 teaspoons (20 mL) of water in a cup and then add all of that mixture to the rest of the water and flour in the saucepan. Stir while bringing it back up to nearly boiling temperature, and then allow it to cool. This mixture should slowly become much thicker \u2014 something like porridge \u2014 because there is more gluten and more chains have been formed (see the photo).<\/p>\n      <div class=\"wp-caption aligncenter\" style=\"width: 547px\">\n        <a>\n          <img alt=\"Thick, white goop in a pot.\" src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/making-magma-viscous2.jpg\" width=\"547\" height=\"410\">\n        <\/a>\n        <div class=\"wp-caption-text\">Figure 3.2.5 Flour-and-water magma experiment.<\/div>\n      <\/div>\n      <p>This is analogous to magma, of course. As we\u2019ll see below, magmas have quite variable contents of silica and therefore have widely varying viscosities (\u201cthicknesses\u201d) during cooling.<\/p>\n      <p>See Appendix 3 for <a href=\"back-matter-005-appendix-3-answers-to-exercises.html#exercisea3.2\">Exercise 3.2 answers<\/a>.<\/p>\n    <\/div>\n  <\/div>\n  <h3>Image Descriptions<\/h3>\n  <p><strong id=\"fig3.6\"><a id=\"fig3.2.1\" href=\"\">Figure 3.2.1 image description:<\/a><\/strong> The average elemental proportions in the Earth\u2019s crust from the largest amount to the smallest amount. Oxygen (46.6%), Silicon (27.7%), Aluminum (8.1%), Iron (5.0%), Calcium (3.6%), Sodium (2.8%), Potassium (2.6%), Magnesium (2.1%), Others (1.5%). <a href=\"#retfig3.2.1\">[Return to Figure 3.2.1]<\/a><\/p>\n  <p><strong id=\"fig3.8\"><a id=\"fig3.2.3\" href=\"\">Figure 3.2.3a image description:<\/a><\/strong> Dry mantle rock is predominately solid. However, its melting point is dependent on the temperature and pressure the rock is under. The higher the pressure (meaning the farther the rock is from the Earth\u2019s surface), the more likely dry mantle rock is going to be solid. Dry mantle rock under extreme pressure requires a much higher temperature to melt than dry mantle rock under less pressure. As pressure drops (meaning as the rock rises towards the Earth\u2019s surface), the required temperature to melt the mantle rock drops as well.<\/p>\n  <p><strong>Figure 3.2.3b image description:<\/strong> In comparison to dry mantle rock, wet mantle rock under the same amount of pressure (at the same distance from the earth\u2019s surface) requires a lower temperature to melt. When liquid is added to dry mantel rock at a pressure and temperature point in which wet mantle rock would be melted, flux melting occurs. <a href=\"#retfig3.2.3\">[Return to Figure 3.2.3]<\/a><\/p>\n  <h3>Media Attributions<\/h3>\n  <ul>\n    <li>Figure 3.2.1, 3.2.2, 3.2.3, 3.2.5: \u00a9 Steven Earle. CC BY.<\/li>\n    <li>Figure 3.2.4: \u201c<a href=\"http:\/\/pubs.usgs.gov\/gip\/dynamic\/Vigil.html\">Cross section<\/a>\u201d by Jos\u00e9 F. Vigil from <em>This Dynamic Planet<\/em> \u2014 a wall map produced jointly by the U.S. Geological Survey, the Smithsonian Institution, and the U.S. Naval Research Laboratory. Adapted by Steven Earle. Public domain.<\/li>\n  <\/ul>\n  <hr class=\"before-footnotes clear\">\n  <div class=\"footnotes\">\n    <ol>\n      <li id=\"footnote-123-1\">Mantle plumes are described in Chapter 4 and mantle convection in Chapter 9. <a href=\"#return-footnote-123-1\" class=\"return-footnote\">\u21b5<\/a><br style=\"line-height:0em;\"><\/li>\n    <\/ol>\n  <\/div>\n  &lt;!-- pb_fixme --&gt;\n<\/div>\n<\/div><div>\n  &lt;!-- pb_fixme --&gt;\n  &lt;!-- pb_fixme --&gt;\n<\/div>\n<\/div>\n","rendered":"<div>\n<div>\n    <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/earths-crust2.png\" alt=\"Elements in the Earth's crust. Long decriptions available\" class=\"wp-image-118\" width=\"700\" height=\"484\" \/><\/p>\n<div class=\"wp-caption-text\" id=\"caption-attachment-121\">Figure 3.2.1 Average elemental proportions in Earth\u2019s crust, which is close to the average composition of magmas within the crust. <a href=\"#fig3.2.1\">[Image Description]<\/a><\/div>\n<\/p><\/div>\n<p>Virtually all of the igneous rocks that we see on Earth are derived from magmas that formed from <strong><span class=\"glossary-term\">partial melting<\/span><\/strong> of existing rock, either in the upper mantle or the crust. Partial melting is what happens when only some parts of a rock melt; it takes place because rocks are not pure materials. Most rocks are made up of several minerals, each of which has a different melting temperature. The wax in a candle is a pure material. If you put some wax into a warm oven (50\u00b0C will do as the melting temperature of most wax is about 40\u00b0C) and leave it there for a while, it will soon start to melt. That\u2019s complete melting, not partial melting. If instead you took a mixture of wax, plastic, aluminum, and glass and put it into the same warm oven, the wax would soon start to melt, but the plastic, aluminum, and glass would not melt (Figure 3.2.2a). That\u2019s partial melting and the result would be solid plastic, aluminum, and glass surrounded by liquid wax (Figure 3.2.2b). If we heat the oven up to around 120\u00b0C, the plastic would melt too and mix with the liquid wax, but the aluminum and glass would remain solid (Figure 3.2.2c). Again this is partial melting. If we separated the wax\/plastic \u201cmagma\u201d from the other components and let it cool, it would eventually harden. As you can see from Figure 3.2.2d, the liquid wax and plastic have mixed, and on cooling, have formed what looks like a single solid substance. It is most likely that this is a very fine-grained mixture of solid wax and solid plastic, but it could also be some other substance that has formed from the combination of the two.<\/p>\n<div class=\"wp-caption aligncenter\" style=\"width: 700px\">\n    <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/pretend-rock-1024x1003-1.png\" alt=\"\" class=\"wp-image-119\" width=\"700\" height=\"686\" \/><\/p>\n<div class=\"wp-caption-text\">Figure 3.2.2 Partial melting of \u201cpretend rock\u201d: (a) the original components of white candle wax, black plastic pipe, green beach glass, and aluminum wire, (b) after heating to 50\u02daC for 30 minutes only the wax has melted, (c) after heating to 120\u02daC for 60 minutes much of the plastic has melted and the two liquids have mixed, (d) the liquid has been separated from the solids and allowed to cool to make a \u201cpretend rock\u201d with a different overall composition.<\/div>\n<\/p><\/div>\n<p>In this example, we partially melted some pretend rock to create some pretend magma. We then separated the magma from the source and allowed it to cool to make a new pretend rock with a composition quite different from the original material (it lacks glass and aluminum).<\/p>\n<p>Of course partial melting in the real world isn\u2019t exactly the same as in our pretend-rock example. The main differences are that rocks are much more complex than the four-component system we used, and the mineral components of most rocks have more similar melting temperatures, so two or more minerals are likely to melt at the same time to varying degrees. Another important difference is that when rocks melt, the process takes thousands to millions of years, not the 90 minutes it took in the pretend-rock example.<\/p>\n<p>Contrary to what one might expect, and contrary to what we did to make our pretend rock, most partial melting of real rock does not involve heating the rock up. The two main mechanisms through which rocks melt are <strong><span class=\"glossary-term\">decompression melting<\/span><\/strong> and <strong><span class=\"glossary-term\">flux melting<\/span><\/strong>. Decompression melting takes place within Earth when a body of rock is held at approximately the same temperature but the pressure is reduced. This happens because the rock is being moved toward the surface, either at a <strong><span class=\"glossary-term\">mantle plume<\/span><\/strong> (a.k.a., hot spot), or in the upwelling part of a mantle convection cell.<a class=\"footnote\" title=\"Mantle plumes are described in Chapter 4 and mantle convection in Chapter 9.\" id=\"return-footnote-123-1\" href=\"#footnote-123-1\"><sup class=\"footnote\">[1]<\/sup><\/a>&nbsp;The mechanism of decompression melting is shown in Figure 3.2.3a. If a rock that is hot enough to be close to its melting point is moved toward the surface, the pressure is reduced, and the rock can pass to the liquid side of its melting curve. At this point, <em>partial<\/em> melting starts to take place. The process of flux melting is shown in Figure 3.2.3b. If a rock is close to its melting point and some water (a flux that promotes melting) is added to the rock, the melting temperature is reduced (solid line versus dotted line), and partial melting starts.<a id=\"retfig3.2.3\" href=\"\"><\/a><\/p>\n<div class=\"wp-caption aligncenter\" style=\"width: 700px\">\n    <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/flux-decompression.png\" alt=\"Graphs describing the melting curve for dry and wet mantle rock. Long description available\" class=\"wp-image-120\" width=\"700\" height=\"317\" \/><\/p>\n<div class=\"wp-caption-text\">Figure 3.2.3 Mechanisms for (a) decompression melting (the rock is moved toward the surface) and (b) flux melting (water is added to the rock) and the melting curve is displaced. <a href=\"#fig3.2.3\">[Image Description]<\/a><\/div>\n<\/p><\/div>\n<p>The partial melting of rock happens in a wide range of situations, most of which are related to plate tectonics. The more important of these are shown in Figure 3.2.3. At both mantle plumes and in the upward parts of convection systems, rock is being moved toward the surface, the pressure is dropping, and at some point, the rock crosses to the liquid side of its melting curve. At subduction zones, water from the wet, subducting oceanic crust is transferred into the overlying hot mantle. This provides the flux needed to lower the melting temperature. In both of these cases, only partial melting takes place\u2014typically only about 10% of the rock melts\u2014and it is always the most silica-rich components of the rock that melt, creating a magma that is more silica-rich than the rock from which it is derived. (By analogy, the melt from our pretend rock is richer in wax and plastic than the \u201crock\u201d from which it was derived.) The magma produced, being less dense than the surrounding rock, moves up through the mantle, and eventually into the crust.<\/p>\n<div class=\"wp-caption aligncenter\" style=\"width: 850px\">\n    <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/magma-formation2-1024x447-1.png\" alt=\"\" class=\"wp-image-121\" width=\"850\" height=\"371\" \/><\/p>\n<div class=\"wp-caption-text\">Figure 3.2.4 Common sites of magma formation in the upper mantle. The black circles are regions of partial melting. The blue arrows represent water being transferred from the subducting plates into the overlying mantle.<\/div>\n<\/p><\/div>\n<p>As it moves toward the surface, and especially when it moves from the mantle into the lower crust, the hot magma interacts with the surrounding rock. This typically leads to partial melting of the surrounding rock because most such magmas are hotter than the melting temperature of crustal rock. (In this case, melting is caused by an increase in temperature.) Again, the more silica-rich parts of the surrounding rock are preferentially melted, and this contributes to an increase in the silica content of the magma.<\/p>\n<p>At very high temperatures (over 1300\u00b0C), most magma is entirely liquid because there is too much energy for the atoms to bond together. As the temperature drops, usually because the magma is slowly moving upward, things start to change. Silicon and oxygen combine to form silica tetrahedra, and then, as cooling continues, the tetrahedra start to link together to make chains (<strong><span class=\"glossary-term\">polymerize<\/span><\/strong>). These silica chains have the important effect of making the magma more viscous (less runny), and as we\u2019ll see in Chapter 4, magma viscosity has significant implications for volcanic eruptions. As the magma continues to cool, crystals start to form.<\/p>\n<div class=\"textbox textbox--exercises\">\n<div class=\"textbox__header\">\n<p>This is an experiment that you can do at home to help you understand the properties of magma. It will only take about 15 minutes, and all you need is half a cup of water and a few tablespoons of flour.<\/p>\n<p>If you\u2019ve ever made gravy, white sauce, or roux, you\u2019ll know how this works.<\/p>\n<p>Place about 1\/2 cup (125 mL) of water in a saucepan over medium heat. Add 2 teaspoons (10 mL) of white flour (this represents silica) and stir while the mixture comes close to boiling. It should thicken like gravy because the gluten in the flour becomes polymerized into chains during this process.<\/p>\n<p>Now you\u2019re going to add more \u201csilica\u201d to see how this changes the viscosity of your magma. Take another 4 teaspoons (20 mL) of flour&nbsp;and mix it thoroughly with about 4 teaspoons (20 mL) of water in a cup and then add all of that mixture to the rest of the water and flour in the saucepan. Stir while bringing it back up to nearly boiling temperature, and then allow it to cool. This mixture should slowly become much thicker \u2014 something like porridge \u2014 because there is more gluten and more chains have been formed (see the photo).<\/p>\n<div class=\"wp-caption aligncenter\" style=\"width: 547px\">\n        <a><br \/>\n          <img loading=\"lazy\" decoding=\"async\" alt=\"Thick, white goop in a pot.\" src=\"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-content\/uploads\/sites\/15\/2021\/09\/making-magma-viscous2.jpg\" width=\"547\" height=\"410\" \/><br \/>\n        <\/a><\/p>\n<div class=\"wp-caption-text\">Figure 3.2.5 Flour-and-water magma experiment.<\/div>\n<\/p><\/div>\n<p>This is analogous to magma, of course. As we\u2019ll see below, magmas have quite variable contents of silica and therefore have widely varying viscosities (\u201cthicknesses\u201d) during cooling.<\/p>\n<p>See Appendix 3 for <a href=\"back-matter-005-appendix-3-answers-to-exercises.html#exercisea3.2\">Exercise 3.2 answers<\/a>.<\/p>\n<\/p><\/div>\n<\/p><\/div>\n<h3>Image Descriptions<\/h3>\n<p><strong id=\"fig3.6\"><a id=\"fig3.2.1\" href=\"\">Figure 3.2.1 image description:<\/a><\/strong> The average elemental proportions in the Earth\u2019s crust from the largest amount to the smallest amount. Oxygen (46.6%), Silicon (27.7%), Aluminum (8.1%), Iron (5.0%), Calcium (3.6%), Sodium (2.8%), Potassium (2.6%), Magnesium (2.1%), Others (1.5%). <a href=\"#retfig3.2.1\">[Return to Figure 3.2.1]<\/a><\/p>\n<p><strong id=\"fig3.8\"><a id=\"fig3.2.3\" href=\"\">Figure 3.2.3a image description:<\/a><\/strong> Dry mantle rock is predominately solid. However, its melting point is dependent on the temperature and pressure the rock is under. The higher the pressure (meaning the farther the rock is from the Earth\u2019s surface), the more likely dry mantle rock is going to be solid. Dry mantle rock under extreme pressure requires a much higher temperature to melt than dry mantle rock under less pressure. As pressure drops (meaning as the rock rises towards the Earth\u2019s surface), the required temperature to melt the mantle rock drops as well.<\/p>\n<p><strong>Figure 3.2.3b image description:<\/strong> In comparison to dry mantle rock, wet mantle rock under the same amount of pressure (at the same distance from the earth\u2019s surface) requires a lower temperature to melt. When liquid is added to dry mantel rock at a pressure and temperature point in which wet mantle rock would be melted, flux melting occurs. <a href=\"#retfig3.2.3\">[Return to Figure 3.2.3]<\/a><\/p>\n<h3>Media Attributions<\/h3>\n<ul>\n<li>Figure 3.2.1, 3.2.2, 3.2.3, 3.2.5: \u00a9 Steven Earle. CC BY.<\/li>\n<li>Figure 3.2.4: \u201c<a href=\"http:\/\/pubs.usgs.gov\/gip\/dynamic\/Vigil.html\">Cross section<\/a>\u201d by Jos\u00e9 F. Vigil from <em>This Dynamic Planet<\/em> \u2014 a wall map produced jointly by the U.S. Geological Survey, the Smithsonian Institution, and the U.S. Naval Research Laboratory. Adapted by Steven Earle. Public domain.<\/li>\n<\/ul>\n<hr class=\"before-footnotes clear\" \/>\n<div class=\"footnotes\">\n<ol>\n<li id=\"footnote-123-1\">Mantle plumes are described in Chapter 4 and mantle convection in Chapter 9. <a href=\"#return-footnote-123-1\" class=\"return-footnote\">\u21b5<\/a><br style=\"line-height:0em;\" \/><\/li>\n<\/ol><\/div>\n<p>  &lt;!&#8211; pb_fixme &#8211;&gt;\n<\/p><\/div>\n<div>\n  &lt;!&#8211; pb_fixme &#8211;&gt;<br \/>\n  &lt;!&#8211; pb_fixme &#8211;&gt;\n<\/div>\n","protected":false},"author":8,"menu_order":28,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-106","chapter","type-chapter","status-publish","hentry"],"part":3,"_links":{"self":[{"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/chapters\/106","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/wp\/v2\/users\/8"}],"version-history":[{"count":1,"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/chapters\/106\/revisions"}],"predecessor-version":[{"id":931,"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/chapters\/106\/revisions\/931"}],"part":[{"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/parts\/3"}],"metadata":[{"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/chapters\/106\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/wp\/v2\/media?parent=106"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/pressbooks\/v2\/chapter-type?post=106"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/wp\/v2\/contributor?post=106"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.ccconline.org\/physicalgeology\/wp-json\/wp\/v2\/license?post=106"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}