z=e^(xy) ln(x y)全微分
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我来试试吧...z=e^xy*cos(x+y)Z'x=ye^xycos(x+y)-e^xysin(x+y)Z'y=xe^xycos(x+y)-e^xysin(x+y)故dZ=[ye^xycos(x+y
可以先在二维坐标中作xy=1的图像,也就是y=1/x.这个图像很容易的,就是在一三象限的反弧线,作好后再扩展到三维坐标系中,就是把线扩展成面,就是两个反弧面.图形就是两个关于Z轴对称的弧面,沿Z轴看就
e^(-xy)-2z+e^z=0-ye^(-xy)-2z'(x)+e^zz'(x)=0z'(x)=ye^(-xy)/(e^z-2)-xe^(-xy)-2z'(y)+e^zz'(y)=0z'(y)=xe
z'x=(-y/x^2)/(y/x)=-1/xz'y=(1/x)/(y/x)=1/ydz=z'xdx+z'ydyu=ln(x^2+y^2+z^2)u'x=2x/(x^2+y^2+z^2)u'y=2y/
Z=e^xy在x处的导函数为ye^(xy)在y处的导函数为xe^(xy)dz=ye^(xy)dx+xe^(xy)dy=2e^2dx+e^2dy
对方程两边求全微分得:(e^z-1)dz+y^3dx+3xy^2dy=0(方法和求导类似)移项,有dz=-(y^3dx+3xy^2dy)/(e^z-1)
δz/δx=1/(xy+x/y)*(y+1/y)=(y²+1)/(xy²+x)=1/xδ^2z/δxδy=δ(δz/δx)/δy=0
dz=d(xyln(xy))=xyd(ln(xy))+ln(xy)d(xy)=xyd(xy)/(xy)+ln(xy)d(xy)=d(xy)+ln(xy)d(xy)=(1+ln(xy))d(xy)=(1
(y^2+2xy-cos(y+z))/(e^z+cos(y+z))再问:没有过程吗?再答:求导:e^z*dz-y^2-2xy+cos(y+z)(1+dz)=0把含有dz的项移到一起:(e^z+cos(
运用函数连续性,化成一元函数求极限x→0,y→2lim[ln(x+e^xy)/x]=x→0lim[ln(x+e^(2x)]/x【0/0型】=x→0lim[ln(1+(x+e^(2x)-1)]/x=x→
答案是1/e当x=1,y=ln(0*1+e)=lne=1所以(0,1)在曲线上.y=ln(xy+e)y'=1/(xy+e)*(y+x*y')y'=y/(xy+e)+x/(xy+e)*y'y'*[1-x
e^(lnx+lny)=e^lnx*e^lny=x*ye^lnxy=xy所以e^(lnx+lny)=e^lnxy所以lnx+lny=lnxy
令x=根号2分之1(x‘-y’)y=根号2分之1(x'+y')z=xy=1/2(x'^2-y'^2)双曲抛物面
z=xy的图形,应该是一种马鞍面.再问:嗯,能说的具体点吗再答:一种马鞍面
求曲面(e^z)-z+xy=4的切平面及法线方程.设曲面方程F(x,y,z)=(e^z)-z+xy-4=0;点M(xo,yo,zo)是该曲面上的任意一点.∂F/∂x=y;
u=ln(xy+z)du=d[ln(xy+z)]/dx*dx+d[ln(xy+z)]/dy*dy+d[ln(xy+z)]/dz*dz=y/(xy+z)*dx+x/(xy+z)*dy+1/(xy+z)*
dy/dx=dy/du*du/dx+dy/dv*dv/dx=v*e^(x+y)+u*y/x=ln(xy)*e^(x+y)+e^(x+y)*y/x=e^(x+y)[ln(xy)+y/x]所以dy=e^(
两边求导得y'·e^y+(y+xy')/(xy)+e^(-x)=0