﻿{"id":4383,"date":"2013-12-18T06:05:33","date_gmt":"2013-12-17T21:05:33","guid":{"rendered":"http:\/\/fujiitoshiki.com\/improvesociety\/?p=4383"},"modified":"2014-08-01T19:14:58","modified_gmt":"2014-08-01T10:14:58","slug":"partial-derivatives","status":"publish","type":"post","link":"https:\/\/www.fujiitoshiki.com\/improvesociety\/?p=4383","title":{"rendered":"Partial derivatives"},"content":{"rendered":"<div class=\"theContentWrap-ccc\"><blockquote>\n<p>The partial derivatives of <img src='https:\/\/s0.wp.com\/latex.php?latex=f%28x%2C+y%29&#038;bg=T&#038;fg=000000&#038;s=0' alt='f(x, y)' title='f(x, y)' class='latex' \/> with respect to x and y are defined by<\/p>\n<p><img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle+%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+x%7D%3D+%5Clim%5Climits_%7Bh+%5Crightarrow+0%7D+%5Cfrac%7Bf%28x+%2B+h%2C+y%29+-+f%28x%2C+y%29%7D%7Bh%7D%5C%5C%5Cvspace%7B0.2+in%7D+++%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+y%7D+%3D+%5Clim%5Climits_%7Bk+%5Crightarrow+0%7D+%5Cfrac%7Bf%28x%2C+y+%2B+k%29+-+f%28x%2C+y%29%7D%7Bk%7D&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle \\frac{\\partial f}{\\partial x}= \\lim\\limits_{h \\rightarrow 0} \\frac{f(x + h, y) - f(x, y)}{h}\\\\\\vspace{0.2 in}   \\frac{\\partial f}{\\partial y} = \\lim\\limits_{k \\rightarrow 0} \\frac{f(x, y + k) - f(x, y)}{k}' title='\\displaystyle \\frac{\\partial f}{\\partial x}= \\lim\\limits_{h \\rightarrow 0} \\frac{f(x + h, y) - f(x, y)}{h}\\\\\\vspace{0.2 in}   \\frac{\\partial f}{\\partial y} = \\lim\\limits_{k \\rightarrow 0} \\frac{f(x, y + k) - f(x, y)}{k}' class='latex' \/><\/p>\n<p>if these limits exist. It&#8217;s often written h = &Delta;x, k = &Delta;y. Note that <img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cpartial+f%2F%5Cpartial+x&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\partial f\/\\partial x' title='\\partial f\/\\partial x' class='latex' \/> is simply the ordinary derivative of f with respect to x keeping y constant, while <img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cpartial+f%2F%5Cpartial+y&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\partial f\/\\partial y' title='\\partial f\/\\partial y' class='latex' \/> is the ordinary derivative of f with respect to y keeping x constant. <\/p>\n<p>Higher derivatives are defined similarly. For example, you have the second order derivatives<\/p>\n<p><img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle++++%5Cfrac%7B%5Cpartial%7D%7B%5Cpartial+x%7D%5Cleft%28%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+x%7D%5Cright%29+%3D+%5Cfrac%7B%5Cpartial%5E2f%7D%7B%5Cpartial+x%5E2%7D%5C%5C%5Cvspace%7B0.2+in%7D+++%5Cfrac%7B%5Cpartial%7D%7B%5Cpartial+x%7D%5Cleft%28%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+y%7D%5Cright%29+%3D+%5Cfrac%7B%5Cpartial%5E2f%7D%7B%5Cpartial+x%5Cpartial+y%7D%5C%5C%5Cvspace%7B0.2+in%7D+++%5Cfrac%7B%5Cpartial%7D%7B%5Cpartial+y%7D%5Cleft%28%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+x%7D%5Cright%29+%3D+%5Cfrac%7B%5Cpartial%5E2f%7D%7B%5Cpartial+y%5Cpartial+x%7D%5C%5C%5Cvspace%7B0.2+in%7D+++%5Cfrac%7B%5Cpartial%7D%7B%5Cpartial+y%7D%5Cleft%28%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+y%7D%5Cright%29+%3D+%5Cfrac%7B%5Cpartial%5E2f%7D%7B%5Cpartial+y%5E2%7D&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle    \\frac{\\partial}{\\partial x}\\left(\\frac{\\partial f}{\\partial x}\\right) = \\frac{\\partial^2f}{\\partial x^2}\\\\\\vspace{0.2 in}   \\frac{\\partial}{\\partial x}\\left(\\frac{\\partial f}{\\partial y}\\right) = \\frac{\\partial^2f}{\\partial x\\partial y}\\\\\\vspace{0.2 in}   \\frac{\\partial}{\\partial y}\\left(\\frac{\\partial f}{\\partial x}\\right) = \\frac{\\partial^2f}{\\partial y\\partial x}\\\\\\vspace{0.2 in}   \\frac{\\partial}{\\partial y}\\left(\\frac{\\partial f}{\\partial y}\\right) = \\frac{\\partial^2f}{\\partial y^2}' title='\\displaystyle    \\frac{\\partial}{\\partial x}\\left(\\frac{\\partial f}{\\partial x}\\right) = \\frac{\\partial^2f}{\\partial x^2}\\\\\\vspace{0.2 in}   \\frac{\\partial}{\\partial x}\\left(\\frac{\\partial f}{\\partial y}\\right) = \\frac{\\partial^2f}{\\partial x\\partial y}\\\\\\vspace{0.2 in}   \\frac{\\partial}{\\partial y}\\left(\\frac{\\partial f}{\\partial x}\\right) = \\frac{\\partial^2f}{\\partial y\\partial x}\\\\\\vspace{0.2 in}   \\frac{\\partial}{\\partial y}\\left(\\frac{\\partial f}{\\partial y}\\right) = \\frac{\\partial^2f}{\\partial y^2}' class='latex' \/><\/p>\n<p>The deviation are sometimes denoted f<sub>x<\/sub> and f<sub>y<\/sub>. In such case f<sub>x<\/sub>(a, b), f<sub>y<\/sub>(a, b) denote these partial derivatives evaluated at (a, b). <\/p>\n<p>The deviations are denoted by f<sub>xx<\/sub>, f<sub>xy<\/sub>, f<sub>yx<\/sub>, f<sub>yy<\/sub> respectively. The second and third results will be the same if f has continuous partial derivatives of second order at least. <\/p>\n<p>The differentiation of f(x, y) is defined as<\/p>\n<p><img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle+df+%3D+%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+x%7Ddx+%2B+%5Cfrac%7B%5Cpartial+f%7D%7B%5Cpartial+y%7Ddy&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle df = \\frac{\\partial f}{\\partial x}dx + \\frac{\\partial f}{\\partial y}dy' title='\\displaystyle df = \\frac{\\partial f}{\\partial x}dx + \\frac{\\partial f}{\\partial y}dy' class='latex' \/><\/p>\n<p>where h = &Delta;x = dx, k = &Delta;y = dy.<\/p>\n<\/blockquote>\n<p><iframe src=\"\/\/rcm-fe.amazon-adsystem.com\/e\/cm?lt1=_blank&#038;bc1=000000&#038;IS2=1&#038;bg1=FFFFFF&#038;fc1=000000&#038;lc1=0000FF&#038;t=fujiitoshiki-22&#038;o=9&#038;p=8&#038;l=as4&#038;m=amazon&#038;f=ifr&#038;ref=ss_til&#038;asins=0071635408\" style=\"width:120px;height:240px;\" scrolling=\"no\" marginwidth=\"0\" marginheight=\"0\" frameborder=\"0\"><\/iframe><\/p>\n<\/div>","protected":false},"excerpt":{"rendered":"<p>The partial derivatives of with respect to x and y are defined by if these limits exist. It&#8217;s often writ &hellip; <a href=\"https:\/\/www.fujiitoshiki.com\/improvesociety\/?p=4383\" class=\"more-link\"><span class=\"screen-reader-text\">&#8220;Partial derivatives&#8221; \u306e<\/span>\u7d9a\u304d\u3092\u8aad\u3080<\/a><\/p>\n","protected":false},"author":1,"featured_media":6040,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_crdt_document":"","_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"categories":[9],"tags":[],"class_list":["post-4383","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-mathematics"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts\/4383","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=4383"}],"version-history":[{"count":15,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts\/4383\/revisions"}],"predecessor-version":[{"id":6069,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts\/4383\/revisions\/6069"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/media\/6040"}],"wp:attachment":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=4383"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=4383"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=4383"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}