{"id":2398,"date":"2020-06-22T02:27:34","date_gmt":"2020-06-22T06:27:34","guid":{"rendered":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/?post_type=chapter&#038;p=2398"},"modified":"2021-07-13T22:17:57","modified_gmt":"2021-07-14T02:17:57","slug":"bonding-explained-with-mo-theory","status":"publish","type":"chapter","link":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/chapter\/bonding-explained-with-mo-theory\/","title":{"raw":"2.8 Bonding explained with MO theory","rendered":"2.8 Bonding explained with MO theory"},"content":{"raw":"<p id=\"fs-idp262340496\">We have examined the basic ideas of bonding, showing that atoms share electrons to form molecules with stable Lewis structures and that we can predict the shapes of those molecules by valence shell electron pair repulsion (VSEPR) theory. These ideas provide an important starting point for understanding chemical bonding. But these models sometimes fall short in their abilities to predict the behavior of real substances. How can we reconcile the geometries of <em data-effect=\"italics\">s, p,<\/em> and <em data-effect=\"italics\">d<\/em> atomic orbitals with molecular shapes that show angles like 120\u00b0 and 109.5\u00b0? Furthermore, we know that electrons and magnetic behavior are related through electromagnetic fields. Both N<sub>2<\/sub> and O<sub>2<\/sub> have fairly similar Lewis structures that contain lone pairs of electrons.<\/p>\r\n<span id=\"fs-idp82346208\" class=\"scaled-down\" data-type=\"media\" data-alt=\"Two Lewis diagrams are shown. The diagram on the left shows two nitrogen atoms, represented by the letter N connected by three lines and with a lone pair of electrons on each end of the structure. The diagram on the right shows two oxygen atoms, depicted by the letter O, connected by two lines. Two pairs of electrons surround each oxygen to the top and ends of the structure.\"><img class=\"aligncenter\" src=\"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-content\/uploads\/sites\/989\/2020\/04\/CNX_Chem_08_00_N2O2Lewis_img-1-1.jpg\" alt=\"Two Lewis diagrams are shown. The diagram on the left shows two nitrogen atoms, represented by the letter N connected by three lines and with a lone pair of electrons on each end of the structure. The diagram on the right shows two oxygen atoms, depicted by the letter O, connected by two lines. Two pairs of electrons surround each oxygen to the top and ends of the structure.\" width=\"325\" height=\"53\" data-media-type=\"image\/jpeg\" \/><\/span>\r\n<p id=\"fs-idm1216176\">Yet oxygen demonstrates very different magnetic behavior than nitrogen. We can pour liquid nitrogen through a magnetic field with no visible interactions, while liquid oxygen (shown in <a class=\"autogenerated-content\" href=\"#CNX_Chem_08_00_LiqO2\">(Figure 1.8.1)<\/a>) is attracted to the magnet and floats in the magnetic field. We need to understand the additional concepts of valence bond theory, orbital hybridization, and molecular orbital theory to understand these observations.<\/p>\r\n\r\n<div class=\"bc-figcaption figcaption\"><\/div>\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"1300\"]<img src=\"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-content\/uploads\/sites\/989\/2020\/04\/CNX_Chem_08_00_LiqO2-1.jpg\" alt=\"A pitcher is shown pouring liquid oxygen through the gap between two magnets, where it has formed a solid disk. A call out box near the stream of liquid oxygen shows an image of six pairs of spheres, spread apart from one another. Another call out box near the solid disk shows ten pairs of spheres much closer together.\" width=\"1300\" height=\"600\" data-media-type=\"image\/jpeg\" \/> <strong>Figure 2.8.1 - Oxygen molecules orient randomly most of the time, as shown in the top magnified view. However, when we pour liquid oxygen through a magnet, the molecules line up with the magnetic field, and the attraction allows them to stay suspended between the poles of the magnet where the magnetic field is strongest. Other diatomic molecules (like N<sub>2<\/sub>) flow past the magnet. The detailed explanation of bonding described in this chapter allows us to understand this phenomenon. (credit: modification of work by Jefferson Lab)<\/strong>[\/caption]\r\n\r\nBased on the MO theory, covalent (single and multiple) bonds can be explained.\u00a0 In addition to providing an explanation for the shape of the resulting molecule and the magnetic properties, MO theory can be used to explain multiple oxidation states for transition metal ions.\u00a0 The d-d transitions and colors exhibited by compounds of the d-block metals can be explained using the MO theory.","rendered":"<p id=\"fs-idp262340496\">We have examined the basic ideas of bonding, showing that atoms share electrons to form molecules with stable Lewis structures and that we can predict the shapes of those molecules by valence shell electron pair repulsion (VSEPR) theory. These ideas provide an important starting point for understanding chemical bonding. But these models sometimes fall short in their abilities to predict the behavior of real substances. How can we reconcile the geometries of <em data-effect=\"italics\">s, p,<\/em> and <em data-effect=\"italics\">d<\/em> atomic orbitals with molecular shapes that show angles like 120\u00b0 and 109.5\u00b0? Furthermore, we know that electrons and magnetic behavior are related through electromagnetic fields. Both N<sub>2<\/sub> and O<sub>2<\/sub> have fairly similar Lewis structures that contain lone pairs of electrons.<\/p>\n<p><span id=\"fs-idp82346208\" class=\"scaled-down\" data-type=\"media\" data-alt=\"Two Lewis diagrams are shown. The diagram on the left shows two nitrogen atoms, represented by the letter N connected by three lines and with a lone pair of electrons on each end of the structure. The diagram on the right shows two oxygen atoms, depicted by the letter O, connected by two lines. Two pairs of electrons surround each oxygen to the top and ends of the structure.\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-content\/uploads\/sites\/989\/2020\/04\/CNX_Chem_08_00_N2O2Lewis_img-1-1.jpg\" alt=\"Two Lewis diagrams are shown. The diagram on the left shows two nitrogen atoms, represented by the letter N connected by three lines and with a lone pair of electrons on each end of the structure. The diagram on the right shows two oxygen atoms, depicted by the letter O, connected by two lines. Two pairs of electrons surround each oxygen to the top and ends of the structure.\" width=\"325\" height=\"53\" data-media-type=\"image\/jpeg\" \/><\/span><\/p>\n<p id=\"fs-idm1216176\">Yet oxygen demonstrates very different magnetic behavior than nitrogen. We can pour liquid nitrogen through a magnetic field with no visible interactions, while liquid oxygen (shown in <a class=\"autogenerated-content\" href=\"#CNX_Chem_08_00_LiqO2\">(Figure 1.8.1)<\/a>) is attracted to the magnet and floats in the magnetic field. We need to understand the additional concepts of valence bond theory, orbital hybridization, and molecular orbital theory to understand these observations.<\/p>\n<div class=\"bc-figcaption figcaption\"><\/div>\n<figure style=\"width: 1300px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-content\/uploads\/sites\/989\/2020\/04\/CNX_Chem_08_00_LiqO2-1.jpg\" alt=\"A pitcher is shown pouring liquid oxygen through the gap between two magnets, where it has formed a solid disk. A call out box near the stream of liquid oxygen shows an image of six pairs of spheres, spread apart from one another. Another call out box near the solid disk shows ten pairs of spheres much closer together.\" width=\"1300\" height=\"600\" data-media-type=\"image\/jpeg\" \/><figcaption class=\"wp-caption-text\"><strong>Figure 2.8.1 &#8211; Oxygen molecules orient randomly most of the time, as shown in the top magnified view. However, when we pour liquid oxygen through a magnet, the molecules line up with the magnetic field, and the attraction allows them to stay suspended between the poles of the magnet where the magnetic field is strongest. Other diatomic molecules (like N<sub>2<\/sub>) flow past the magnet. The detailed explanation of bonding described in this chapter allows us to understand this phenomenon. (credit: modification of work by Jefferson Lab)<\/strong><\/figcaption><\/figure>\n<p>Based on the MO theory, covalent (single and multiple) bonds can be explained.\u00a0 In addition to providing an explanation for the shape of the resulting molecule and the magnetic properties, MO theory can be used to explain multiple oxidation states for transition metal ions.\u00a0 The d-d transitions and colors exhibited by compounds of the d-block metals can be explained using the MO theory.<\/p>\n","protected":false},"author":928,"menu_order":9,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-2398","chapter","type-chapter","status-publish","hentry"],"part":1620,"_links":{"self":[{"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/chapters\/2398","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/wp\/v2\/users\/928"}],"version-history":[{"count":5,"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/chapters\/2398\/revisions"}],"predecessor-version":[{"id":3596,"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/chapters\/2398\/revisions\/3596"}],"part":[{"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/parts\/1620"}],"metadata":[{"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/chapters\/2398\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/wp\/v2\/media?parent=2398"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/pressbooks\/v2\/chapter-type?post=2398"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/wp\/v2\/contributor?post=2398"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/inorganicchemistrychem250\/wp-json\/wp\/v2\/license?post=2398"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}