{"id":27,"date":"2017-11-14T13:47:05","date_gmt":"2017-11-14T18:47:05","guid":{"rendered":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/back-matter\/mathematical-formulas\/"},"modified":"2017-11-14T13:47:05","modified_gmt":"2017-11-14T18:47:05","slug":"mathematical-formulas","status":"publish","type":"back-matter","link":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/back-matter\/mathematical-formulas\/","title":{"raw":"Mathematical Formulas","rendered":"Mathematical Formulas"},"content":{"raw":"<p id=\"fs-id1171238709218\"><strong>Quadratic formula<\/strong><\/p><p id=\"fs-id1171241118332\">If [latex]a{x}^{2}+bx+c=0,[\/latex] then [latex]x=\\frac{\\text{\u2212}b\u00b1\\sqrt{{b}^{2}-4ac}}{2a}[\/latex]<\/p><table id=\"fs-id1171241121579\" summary=\"This table has three columns and four rows. The entry in the first row are: Triangle of base b and height h, Area equal to half bh. The third cell in the first row is blank. the second row has the following entries: Circle of radius r, Circumference equal to 2 pi r, Area equal to pi r squared. The third row has the following entries: Sphere of radius r, Surface area equal to 4 pi r squared, volume equal to 4 by 3 pi r cubed. The fourth row has the following entries: Cylinder of radius r and height h, Area of curved surface equal to 2 pi r h, Volume equal to pi r squared h.\"><caption><span>Geometry<\/span><\/caption><thead><tr valign=\"top\"><th>Triangle of base [latex]b[\/latex] and height [latex]h[\/latex]<\/th><th>Area [latex]=\\frac{1}{2}bh[\/latex]<\/th><th><\/th><\/tr><\/thead><tbody><tr valign=\"top\"><td>Circle of radius [latex]r[\/latex]<\/td><td>Circumference [latex]=2\\pi r[\/latex]<\/td><td>Area [latex]=\\pi {r}^{2}[\/latex]<\/td><\/tr><tr valign=\"top\"><td>Sphere of radius [latex]r[\/latex]<\/td><td>Surface area [latex]=4\\pi {r}^{2}[\/latex]<\/td><td>Volume [latex]=\\frac{4}{3}\\pi {r}^{3}[\/latex]<\/td><\/tr><tr valign=\"top\"><td>Cylinder of radius [latex]r[\/latex] and height [latex]h[\/latex]<\/td><td>Area of curved surface [latex]=2\\pi rh[\/latex]<\/td><td>Volume [latex]=\\pi {r}^{2}h[\/latex]<\/td><\/tr><\/tbody><\/table><p id=\"fs-id1171241192710\"><strong>Trigonometry<\/strong><\/p><p id=\"fs-id1171241320523\"><em>Trigonometric Identities<\/em><\/p><ol id=\"fs-id1171241111731\" type=\"1\"><li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta =1\\text{\/}\\text{csc}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta =1\\text{\/}\\text{sec}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\theta =1\\text{\/}\\text{cot}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{sin}\\left({90}^{0}-\\theta \\right)=\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{cos}\\left({90}^{0}-\\theta \\right)=\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{tan}\\left({90}^{0}-\\theta \\right)=\\text{cot}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]{\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta +{\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta =1[\/latex]<\/li><li>[latex]{\\text{sec}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta -{\\text{tan}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta =1[\/latex]<\/li><li>[latex]\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\theta =\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta \\text{\/}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{sin}\\left(\\alpha \u00b1\\beta \\right)=\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\beta \u00b1\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta [\/latex]<\/li><li>[latex]\\text{cos}\\left(\\alpha \u00b1\\beta \\right)=\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\beta \\mp \\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta [\/latex]<\/li><li>[latex]\\text{tan}\\left(\\alpha \u00b1\\beta \\right)=\\frac{\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\alpha \u00b1\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\beta }{1\\mp \\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\beta }[\/latex]<\/li><li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}2\\theta =2\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta \\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}2\\theta ={\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta -{\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta =2\\phantom{\\rule{0.2em}{0ex}}{\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta -1=1-2\\phantom{\\rule{0.2em}{0ex}}{\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta [\/latex]<\/li><li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha +\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta =2\\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\frac{1}{2}\\left(\\alpha +\\beta \\right)\\text{cos}\\frac{1}{2}\\left(\\alpha -\\beta \\right)[\/latex]<\/li><li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\alpha +\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\beta =2\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\frac{1}{2}\\left(\\alpha +\\beta \\right)\\text{cos}\\frac{1}{2}\\left(\\alpha -\\beta \\right)[\/latex]<\/li><\/ol><p id=\"fs-id1171241012787\"><em>Triangles<\/em><\/p><ol id=\"fs-id1171241129165\" type=\"1\"><li>Law of sines: [latex]\\frac{a}{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha }=\\frac{b}{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta }=\\frac{c}{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\gamma }[\/latex]<\/li><li>Law of cosines: [latex]{c}^{2}={a}^{2}+{b}^{2}-2ab\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\gamma [\/latex]<div><br \/><\/div>\n<span id=\"fs-id1171241119734\"><img src=\"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-content\/uploads\/sites\/287\/2017\/11\/CNX_UPhysics_00_EE_Triangle1_img.jpg\" alt=\"Figure shows a triangle with three dissimilar sides labeled a, b and c. All three angles of the triangle are acute angles. The angle between b and c is alpha, the angle between a and c is beta and the angle between a and b is gamma.\" \/><\/span><\/li><li>Pythagorean theorem: [latex]{a}^{2}+{b}^{2}={c}^{2}[\/latex]<div><br \/><\/div>\n<span id=\"fs-id1171241024569\"><img src=\"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-content\/uploads\/sites\/287\/2017\/11\/CNX_UPhysics_00_EE_Triangle2_img.jpg\" alt=\"Figure shows a right triangle. Its three sides are labeled a, b and c with c being the hypotenuse. The angle between a and c is labeled theta.\" \/><\/span><\/li><\/ol><p id=\"fs-id1171241190802\"><strong>Series expansions<\/strong><\/p><ol id=\"fs-id1171241016910\" type=\"1\"><li>Binomial theorem: [latex]{\\left(a+b\\right)}^{n}={a}^{n}+n{a}^{n-1}b+\\frac{n\\left(n-1\\right){a}^{n-2}{b}^{2}}{2\\text{!}}+\\frac{n\\left(n-1\\right)\\left(n-2\\right){a}^{n-3}{b}^{3}}{3\\text{!}}+\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li><li>[latex]{\\left(1\u00b1x\\right)}^{n}=1\u00b1\\frac{nx}{1\\text{!}}+\\frac{n\\left(n-1\\right){x}^{2}}{2\\text{!}}\u00b1\\text{\u00b7\u00b7\u00b7}\\left({x}^{2}&lt;1\\right)[\/latex]<\/li><li>[latex]{\\left(1\u00b1x\\right)}^{\\text{\u2212}n}=1\\mp \\frac{nx}{1\\text{!}}+\\frac{n\\left(n+1\\right){x}^{2}}{2\\text{!}}\\mp \\text{\u00b7\u00b7\u00b7}\\left({x}^{2}&lt;1\\right)[\/latex]<\/li><li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x=x-\\frac{{x}^{3}}{3\\text{!}}+\\frac{{x}^{5}}{5\\text{!}}-\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li><li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x=1-\\frac{{x}^{2}}{2\\text{!}}+\\frac{{x}^{4}}{4\\text{!}}-\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li><li>[latex]\\text{tan}\\phantom{\\rule{0.2em}{0ex}}x=x+\\frac{{x}^{3}}{3}+\\frac{2{x}^{5}}{15}+\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li><li>[latex]{e}^{x}=1+x+\\frac{{x}^{2}}{2\\text{!}}+\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li><li>[latex]\\text{ln}\\left(1+x\\right)=x-\\frac{1}{2}{x}^{2}+\\frac{1}{3}{x}^{3}-\\text{\u00b7\u00b7\u00b7}\\left(|x|&lt;1\\right)[\/latex]<\/li><\/ol><p id=\"fs-id1171241003878\"><strong>Derivatives<\/strong><\/p><ol id=\"fs-id1171241165751\" type=\"1\"><li>[latex]\\frac{d}{dx}\\left[af\\left(x\\right)\\right]=a\\frac{d}{dx}f\\left(x\\right)[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\left[f\\left(x\\right)+g\\left(x\\right)\\right]=\\frac{d}{dx}f\\left(x\\right)+\\frac{d}{dx}g\\left(x\\right)[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\left[f\\left(x\\right)g\\left(x\\right)\\right]=f\\left(x\\right)\\frac{d}{dx}g\\left(x\\right)+g\\left(x\\right)\\frac{d}{dx}f\\left(x\\right)[\/latex]<\/li><li>[latex]\\frac{d}{dx}f\\left(u\\right)=\\left[\\frac{d}{du}f\\left(u\\right)\\right]\\frac{du}{dx}[\/latex]<\/li><li>[latex]\\frac{d}{dx}{x}^{m}=m{x}^{m-1}[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x=\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x=\\text{\u2212}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{tan}\\phantom{\\rule{0.2em}{0ex}}x={\\text{sec}}^{2}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{cot}\\phantom{\\rule{0.2em}{0ex}}x=\\text{\u2212}{\\text{csc}}^{2}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{sec}\\phantom{\\rule{0.2em}{0ex}}x=\\text{tan}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}\\text{sec}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{csc}\\phantom{\\rule{0.2em}{0ex}}x=\\text{\u2212}\\text{cot}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}\\text{csc}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\frac{d}{dx}{e}^{x}={e}^{x}[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{ln}\\phantom{\\rule{0.2em}{0ex}}x=\\frac{1}{x}[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}{\\text{sin}}^{-1}\\phantom{\\rule{0.2em}{0ex}}x=\\frac{1}{\\sqrt{1-{x}^{2}}}[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}{\\text{cos}}^{-1}x=-\\frac{1}{\\sqrt{1-{x}^{2}}}[\/latex]<\/li><li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}{\\text{tan}}^{-1}x=-\\frac{1}{1+{x}^{2}}[\/latex]<\/li><\/ol><p id=\"fs-id1171241165019\"><strong>Integrals<\/strong><\/p><ol id=\"fs-id1171241242695\" type=\"1\"><li>[latex]\\int af\\left(x\\right)dx=a\\int f\\left(x\\right)dx[\/latex]<\/li><li>[latex]\\int \\left[f\\left(x\\right)+g\\left(x\\right)\\right]dx=\\int f\\left(x\\right)dx+\\int g\\left(x\\right)dx[\/latex]<\/li><li>[latex]\\begin{array}{cc}\\hfill \\int {x}^{m}dx&amp; =\\frac{{x}^{m+1}}{m+1}\\phantom{\\rule{0.2em}{0ex}}\\left(m\\ne \\text{\u2212}1\\right)\\hfill \\\\ &amp; =\\text{ln}\\phantom{\\rule{0.2em}{0ex}}x\\left(m=-1\\right)\\hfill \\end{array}[\/latex]<\/li><li>[latex]\\int \\text{sin}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}dx=\\text{\u2212}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\int \\text{cos}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}dx=\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li><li>[latex]\\int \\text{tan}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}dx=\\text{ln}|\\text{sec}\\phantom{\\rule{0.2em}{0ex}}x|[\/latex]<\/li><li>[latex]\\int {\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}-\\frac{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}2ax}{4a}[\/latex]<\/li><li>[latex]\\int {\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}+\\frac{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}2ax}{4a}[\/latex]<\/li><li>[latex]\\int \\text{sin}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=-\\frac{\\text{cos}2ax}{4a}[\/latex]<\/li><li>[latex]\\int {e}^{ax}\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{1}{a}{e}^{ax}[\/latex]<\/li><li>[latex]\\int x{e}^{ax}dx=\\frac{{e}^{ax}}{{a}^{2}}\\left(ax-1\\right)[\/latex]<\/li><li>[latex]\\int \\text{ln}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=x\\phantom{\\rule{0.2em}{0ex}}\\text{ln}\\phantom{\\rule{0.2em}{0ex}}ax-x[\/latex]<\/li><li>[latex]\\int \\frac{dx}{{a}^{2}+{x}^{2}}=\\frac{1}{a}\\phantom{\\rule{0.2em}{0ex}}{\\text{tan}}^{-1}\\frac{x}{a}[\/latex]<\/li><li>[latex]\\int \\frac{dx}{{a}^{2}-{x}^{2}}=\\frac{1}{2a}\\phantom{\\rule{0.2em}{0ex}}\\text{ln}|\\frac{x+a}{x-a}|[\/latex]<\/li><li>[latex]\\int \\frac{dx}{\\sqrt{{a}^{2}+{x}^{2}}}={\\text{sinh}}^{-1}\\frac{x}{a}[\/latex]<\/li><li>[latex]\\int \\frac{dx}{\\sqrt{{a}^{2}-{x}^{2}}}={\\text{sin}}^{-1}\\frac{x}{a}[\/latex]<\/li><li>[latex]\\int \\sqrt{{a}^{2}+{x}^{2}}\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}\\sqrt{{a}^{2}+{x}^{2}}+\\frac{{a}^{2}}{2}\\phantom{\\rule{0.2em}{0ex}}{\\text{sinh}}^{-1}\\frac{x}{a}[\/latex]<\/li><li>[latex]\\int \\sqrt{{a}^{2}-{x}^{2}}\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}\\sqrt{{a}^{2}-{x}^{2}}+\\frac{{a}^{2}}{2}\\phantom{\\rule{0.2em}{0ex}}{\\text{sin}}^{-1}\\frac{x}{a}[\/latex]<\/li><\/ol>","rendered":"<p id=\"fs-id1171238709218\"><strong>Quadratic formula<\/strong><\/p>\n<p id=\"fs-id1171241118332\">If [latex]a{x}^{2}+bx+c=0,[\/latex] then [latex]x=\\frac{\\text{\u2212}b\u00b1\\sqrt{{b}^{2}-4ac}}{2a}[\/latex]<\/p>\n<table id=\"fs-id1171241121579\" summary=\"This table has three columns and four rows. The entry in the first row are: Triangle of base b and height h, Area equal to half bh. The third cell in the first row is blank. the second row has the following entries: Circle of radius r, Circumference equal to 2 pi r, Area equal to pi r squared. The third row has the following entries: Sphere of radius r, Surface area equal to 4 pi r squared, volume equal to 4 by 3 pi r cubed. The fourth row has the following entries: Cylinder of radius r and height h, Area of curved surface equal to 2 pi r h, Volume equal to pi r squared h.\">\n<caption><span>Geometry<\/span><\/caption>\n<thead>\n<tr valign=\"top\">\n<th>Triangle of base [latex]b[\/latex] and height [latex]h[\/latex]<\/th>\n<th>Area [latex]=\\frac{1}{2}bh[\/latex]<\/th>\n<th><\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr valign=\"top\">\n<td>Circle of radius [latex]r[\/latex]<\/td>\n<td>Circumference [latex]=2\\pi r[\/latex]<\/td>\n<td>Area [latex]=\\pi {r}^{2}[\/latex]<\/td>\n<\/tr>\n<tr valign=\"top\">\n<td>Sphere of radius [latex]r[\/latex]<\/td>\n<td>Surface area [latex]=4\\pi {r}^{2}[\/latex]<\/td>\n<td>Volume [latex]=\\frac{4}{3}\\pi {r}^{3}[\/latex]<\/td>\n<\/tr>\n<tr valign=\"top\">\n<td>Cylinder of radius [latex]r[\/latex] and height [latex]h[\/latex]<\/td>\n<td>Area of curved surface [latex]=2\\pi rh[\/latex]<\/td>\n<td>Volume [latex]=\\pi {r}^{2}h[\/latex]<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p id=\"fs-id1171241192710\"><strong>Trigonometry<\/strong><\/p>\n<p id=\"fs-id1171241320523\"><em>Trigonometric Identities<\/em><\/p>\n<ol id=\"fs-id1171241111731\" type=\"1\">\n<li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta =1\\text{\/}\\text{csc}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta =1\\text{\/}\\text{sec}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\theta =1\\text{\/}\\text{cot}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{sin}\\left({90}^{0}-\\theta \\right)=\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{cos}\\left({90}^{0}-\\theta \\right)=\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{tan}\\left({90}^{0}-\\theta \\right)=\\text{cot}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]{\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta +{\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta =1[\/latex]<\/li>\n<li>[latex]{\\text{sec}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta -{\\text{tan}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta =1[\/latex]<\/li>\n<li>[latex]\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\theta =\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta \\text{\/}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{sin}\\left(\\alpha \u00b1\\beta \\right)=\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\beta \u00b1\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta[\/latex]<\/li>\n<li>[latex]\\text{cos}\\left(\\alpha \u00b1\\beta \\right)=\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\beta \\mp \\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta[\/latex]<\/li>\n<li>[latex]\\text{tan}\\left(\\alpha \u00b1\\beta \\right)=\\frac{\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\alpha \u00b1\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\beta }{1\\mp \\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\alpha \\phantom{\\rule{0.2em}{0ex}}\\text{tan}\\phantom{\\rule{0.2em}{0ex}}\\beta }[\/latex]<\/li>\n<li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}2\\theta =2\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\theta \\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}2\\theta ={\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta -{\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta =2\\phantom{\\rule{0.2em}{0ex}}{\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta -1=1-2\\phantom{\\rule{0.2em}{0ex}}{\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}\\theta[\/latex]<\/li>\n<li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha +\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta =2\\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\frac{1}{2}\\left(\\alpha +\\beta \\right)\\text{cos}\\frac{1}{2}\\left(\\alpha -\\beta \\right)[\/latex]<\/li>\n<li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\alpha +\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\beta =2\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\frac{1}{2}\\left(\\alpha +\\beta \\right)\\text{cos}\\frac{1}{2}\\left(\\alpha -\\beta \\right)[\/latex]<\/li>\n<\/ol>\n<p id=\"fs-id1171241012787\"><em>Triangles<\/em><\/p>\n<ol id=\"fs-id1171241129165\" type=\"1\">\n<li>Law of sines: [latex]\\frac{a}{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\alpha }=\\frac{b}{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\beta }=\\frac{c}{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}\\gamma }[\/latex]<\/li>\n<li>Law of cosines: [latex]{c}^{2}={a}^{2}+{b}^{2}-2ab\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}\\gamma[\/latex]\n<div><\/div>\n<p><span id=\"fs-id1171241119734\"><img decoding=\"async\" src=\"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-content\/uploads\/sites\/287\/2017\/11\/CNX_UPhysics_00_EE_Triangle1_img.jpg\" alt=\"Figure shows a triangle with three dissimilar sides labeled a, b and c. All three angles of the triangle are acute angles. The angle between b and c is alpha, the angle between a and c is beta and the angle between a and b is gamma.\" \/><\/span><\/li>\n<li>Pythagorean theorem: [latex]{a}^{2}+{b}^{2}={c}^{2}[\/latex]\n<div><\/div>\n<p><span id=\"fs-id1171241024569\"><img decoding=\"async\" src=\"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-content\/uploads\/sites\/287\/2017\/11\/CNX_UPhysics_00_EE_Triangle2_img.jpg\" alt=\"Figure shows a right triangle. Its three sides are labeled a, b and c with c being the hypotenuse. The angle between a and c is labeled theta.\" \/><\/span><\/li>\n<\/ol>\n<p id=\"fs-id1171241190802\"><strong>Series expansions<\/strong><\/p>\n<ol id=\"fs-id1171241016910\" type=\"1\">\n<li>Binomial theorem: [latex]{\\left(a+b\\right)}^{n}={a}^{n}+n{a}^{n-1}b+\\frac{n\\left(n-1\\right){a}^{n-2}{b}^{2}}{2\\text{!}}+\\frac{n\\left(n-1\\right)\\left(n-2\\right){a}^{n-3}{b}^{3}}{3\\text{!}}+\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li>\n<li>[latex]{\\left(1\u00b1x\\right)}^{n}=1\u00b1\\frac{nx}{1\\text{!}}+\\frac{n\\left(n-1\\right){x}^{2}}{2\\text{!}}\u00b1\\text{\u00b7\u00b7\u00b7}\\left({x}^{2}<1\\right)[\/latex]<\/li>\n<li>[latex]{\\left(1\u00b1x\\right)}^{\\text{\u2212}n}=1\\mp \\frac{nx}{1\\text{!}}+\\frac{n\\left(n+1\\right){x}^{2}}{2\\text{!}}\\mp \\text{\u00b7\u00b7\u00b7}\\left({x}^{2}<1\\right)[\/latex]<\/li>\n<li>[latex]\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x=x-\\frac{{x}^{3}}{3\\text{!}}+\\frac{{x}^{5}}{5\\text{!}}-\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li>\n<li>[latex]\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x=1-\\frac{{x}^{2}}{2\\text{!}}+\\frac{{x}^{4}}{4\\text{!}}-\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li>\n<li>[latex]\\text{tan}\\phantom{\\rule{0.2em}{0ex}}x=x+\\frac{{x}^{3}}{3}+\\frac{2{x}^{5}}{15}+\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li>\n<li>[latex]{e}^{x}=1+x+\\frac{{x}^{2}}{2\\text{!}}+\\text{\u00b7\u00b7\u00b7}[\/latex]<\/li>\n<li>[latex]\\text{ln}\\left(1+x\\right)=x-\\frac{1}{2}{x}^{2}+\\frac{1}{3}{x}^{3}-\\text{\u00b7\u00b7\u00b7}\\left(|x|<1\\right)[\/latex]<\/li>\n<\/ol>\n<p id=\"fs-id1171241003878\"><strong>Derivatives<\/strong><\/p>\n<ol id=\"fs-id1171241165751\" type=\"1\">\n<li>[latex]\\frac{d}{dx}\\left[af\\left(x\\right)\\right]=a\\frac{d}{dx}f\\left(x\\right)[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\left[f\\left(x\\right)+g\\left(x\\right)\\right]=\\frac{d}{dx}f\\left(x\\right)+\\frac{d}{dx}g\\left(x\\right)[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\left[f\\left(x\\right)g\\left(x\\right)\\right]=f\\left(x\\right)\\frac{d}{dx}g\\left(x\\right)+g\\left(x\\right)\\frac{d}{dx}f\\left(x\\right)[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}f\\left(u\\right)=\\left[\\frac{d}{du}f\\left(u\\right)\\right]\\frac{du}{dx}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}{x}^{m}=m{x}^{m-1}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x=\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x=\\text{\u2212}\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{tan}\\phantom{\\rule{0.2em}{0ex}}x={\\text{sec}}^{2}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{cot}\\phantom{\\rule{0.2em}{0ex}}x=\\text{\u2212}{\\text{csc}}^{2}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{sec}\\phantom{\\rule{0.2em}{0ex}}x=\\text{tan}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}\\text{sec}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{csc}\\phantom{\\rule{0.2em}{0ex}}x=\\text{\u2212}\\text{cot}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}\\text{csc}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}{e}^{x}={e}^{x}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}\\text{ln}\\phantom{\\rule{0.2em}{0ex}}x=\\frac{1}{x}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}{\\text{sin}}^{-1}\\phantom{\\rule{0.2em}{0ex}}x=\\frac{1}{\\sqrt{1-{x}^{2}}}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}{\\text{cos}}^{-1}x=-\\frac{1}{\\sqrt{1-{x}^{2}}}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx}\\phantom{\\rule{0.2em}{0ex}}{\\text{tan}}^{-1}x=-\\frac{1}{1+{x}^{2}}[\/latex]<\/li>\n<\/ol>\n<p id=\"fs-id1171241165019\"><strong>Integrals<\/strong><\/p>\n<ol id=\"fs-id1171241242695\" type=\"1\">\n<li>[latex]\\int af\\left(x\\right)dx=a\\int f\\left(x\\right)dx[\/latex]<\/li>\n<li>[latex]\\int \\left[f\\left(x\\right)+g\\left(x\\right)\\right]dx=\\int f\\left(x\\right)dx+\\int g\\left(x\\right)dx[\/latex]<\/li>\n<li>[latex]\\begin{array}{cc}\\hfill \\int {x}^{m}dx& =\\frac{{x}^{m+1}}{m+1}\\phantom{\\rule{0.2em}{0ex}}\\left(m\\ne \\text{\u2212}1\\right)\\hfill \\\\ & =\\text{ln}\\phantom{\\rule{0.2em}{0ex}}x\\left(m=-1\\right)\\hfill \\end{array}[\/latex]<\/li>\n<li>[latex]\\int \\text{sin}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}dx=\\text{\u2212}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\int \\text{cos}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}dx=\\text{sin}\\phantom{\\rule{0.2em}{0ex}}x[\/latex]<\/li>\n<li>[latex]\\int \\text{tan}\\phantom{\\rule{0.2em}{0ex}}x\\phantom{\\rule{0.2em}{0ex}}dx=\\text{ln}|\\text{sec}\\phantom{\\rule{0.2em}{0ex}}x|[\/latex]<\/li>\n<li>[latex]\\int {\\text{sin}}^{2}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}-\\frac{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}2ax}{4a}[\/latex]<\/li>\n<li>[latex]\\int {\\text{cos}}^{2}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}+\\frac{\\text{sin}\\phantom{\\rule{0.2em}{0ex}}2ax}{4a}[\/latex]<\/li>\n<li>[latex]\\int \\text{sin}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}\\text{cos}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=-\\frac{\\text{cos}2ax}{4a}[\/latex]<\/li>\n<li>[latex]\\int {e}^{ax}\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{1}{a}{e}^{ax}[\/latex]<\/li>\n<li>[latex]\\int x{e}^{ax}dx=\\frac{{e}^{ax}}{{a}^{2}}\\left(ax-1\\right)[\/latex]<\/li>\n<li>[latex]\\int \\text{ln}\\phantom{\\rule{0.2em}{0ex}}ax\\phantom{\\rule{0.2em}{0ex}}dx=x\\phantom{\\rule{0.2em}{0ex}}\\text{ln}\\phantom{\\rule{0.2em}{0ex}}ax-x[\/latex]<\/li>\n<li>[latex]\\int \\frac{dx}{{a}^{2}+{x}^{2}}=\\frac{1}{a}\\phantom{\\rule{0.2em}{0ex}}{\\text{tan}}^{-1}\\frac{x}{a}[\/latex]<\/li>\n<li>[latex]\\int \\frac{dx}{{a}^{2}-{x}^{2}}=\\frac{1}{2a}\\phantom{\\rule{0.2em}{0ex}}\\text{ln}|\\frac{x+a}{x-a}|[\/latex]<\/li>\n<li>[latex]\\int \\frac{dx}{\\sqrt{{a}^{2}+{x}^{2}}}={\\text{sinh}}^{-1}\\frac{x}{a}[\/latex]<\/li>\n<li>[latex]\\int \\frac{dx}{\\sqrt{{a}^{2}-{x}^{2}}}={\\text{sin}}^{-1}\\frac{x}{a}[\/latex]<\/li>\n<li>[latex]\\int \\sqrt{{a}^{2}+{x}^{2}}\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}\\sqrt{{a}^{2}+{x}^{2}}+\\frac{{a}^{2}}{2}\\phantom{\\rule{0.2em}{0ex}}{\\text{sinh}}^{-1}\\frac{x}{a}[\/latex]<\/li>\n<li>[latex]\\int \\sqrt{{a}^{2}-{x}^{2}}\\phantom{\\rule{0.2em}{0ex}}dx=\\frac{x}{2}\\sqrt{{a}^{2}-{x}^{2}}+\\frac{{a}^{2}}{2}\\phantom{\\rule{0.2em}{0ex}}{\\text{sin}}^{-1}\\frac{x}{a}[\/latex]<\/li>\n<\/ol>\n","protected":false},"author":211,"menu_order":6,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"back-matter-type":[],"contributor":[],"license":[],"class_list":["post-27","back-matter","type-back-matter","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/pressbooks\/v2\/back-matter\/27","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/pressbooks\/v2\/back-matter"}],"about":[{"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/wp\/v2\/types\/back-matter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/wp\/v2\/users\/211"}],"version-history":[{"count":0,"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/pressbooks\/v2\/back-matter\/27\/revisions"}],"metadata":[{"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/pressbooks\/v2\/back-matter\/27\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/wp\/v2\/media?parent=27"}],"wp:term":[{"taxonomy":"back-matter-type","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/pressbooks\/v2\/back-matter-type?post=27"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/wp\/v2\/contributor?post=27"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/universityphysicssandbox\/wp-json\/wp\/v2\/license?post=27"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}