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Tutorial 2: Partial Derivatives Engineering Applications of Partial Derivatives

  1. Find the partial derivative (∂f∂y)\displaystyle\left(\frac{\partial f}{\partial y}\right) and (∂f∂x)\displaystyle\left(\frac{\partial f}{\partial x}\right) of these functions using the limit definition

    a. f(x,y)=x2y+2x+y3f(x, y)=x^{2} y+2 x+y^{3}

    Solution
    fx(x,y)=lim⁡h→0f(x+h,y)−f(x,y)h=lim⁡h→0(x+h)2y+2(x+h)+y3−(x2y+2x+y3)h=lim⁡h→0x2y+2xhy+h2y+2x+2h+y3−(x2y+2x+y3)h=lim⁡h→02xhy+h2y+2hh=lim⁡h→02xy+hy+2=2xy+2fy(x,y)=lim⁡h→0f(x,y+h)−f(x,y)h=lim⁡h→0x2(y+h)+2x+(y+h)3−x2y−2x−y3h=lim⁡h→0x2y+x2h+2x+y3+3y2h+3yh2+h3−x2y−2x−y3h=lim⁡h→0x2h+3y2h+3yh2+h3h=lim⁡h→0x2+3y2+3yh+h2=x2+3y2\begin{aligned} f_{x}(x, y) &=\lim _{h \rightarrow 0} \frac{f(x+h, y)-f(x, y)}{h} \\ &=\lim _{h \rightarrow 0} \frac{(x+h)^{2} y+2(x+h)+y^{3}-\left(x^{2} y+2 x+y^{3}\right)}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2} y+2 x h y+h^{2} y+2 x+2 h+y^{3}-\left(x^{2} y+2 x+y^{3}\right)}{h} \\ &=\lim _{h \rightarrow 0} \frac{2 x h y+h^{2} y+2 h}{h} \\ &=\lim _{h \rightarrow 0} 2 x y+h y+2 \\ &=2 x y+2 \\ f_{y}(x, y) &=\lim _{h \rightarrow 0} \frac{f(x, y+h)-f(x, y)}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2}(y+h)+2 x+(y+h)^{3}-x^{2} y-2 x-y^{3}}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2} y+x^{2} h+2 x+y^{3}+3 y^{2} h+3 y h^{2}+h^{3}-x^{2} y-2 x-y^{3}}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2} h+3 y^{2} h+3 y h^{2}+h^{3}}{h} \\ &=\lim _{h \rightarrow 0} x^{2}+3 y^{2}+3 y h+h^{2} \\ &=x^{2}+3 y^{2} \end{aligned}

    b. f(x,y)=x2−4xy+y2f(x, y)=x^{2}-4 x y+y^{2}

    Solution

    Using the definition,

    fx(x,y)=lim⁡h→0f(x+h,y)−f(x,y)h=lim⁡h→0(x+h)2−4(x+h)y+y2−(x2−4xy+y2)h=lim⁡h→0x2+2xh+h2−4xy−4hy+y2−(x2−4xy+y2)h=lim⁡h→02xh+h2−4hyh=lim⁡h→0(2x+h−4y)=2x−4y\begin{aligned} f_{x}(x, y) &=\lim _{h \rightarrow 0} \frac{f(x+h, y)-f(x, y)}{h} \\ &=\lim _{h \rightarrow 0} \frac{(x+h)^{2}-4(x+h) y+y^{2}-\left(x^{2}-4 x y+y^{2}\right)}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2}+2 x h+h^{2}-4 x y-4 h y+y^{2}-\left(x^{2}-4 x y+y^{2}\right)}{h} \\ &=\lim _{h \rightarrow 0} \frac{2 x h+h^{2}-4 h y}{h} \\ &=\lim _{h \rightarrow 0}(2 x+h-4 y) \\ &=2 x-4 y \end{aligned}

    Similarly,

    fy(x,y)=lim⁡h→0f(x,y+h)−f(x,y)h=lim⁡h→0x2−4x(y+h)+(y+h)2−(x2−4xy+y2)h=lim⁡h→0x2−4xy−4xh+y2+2yh+h2−(x2−4xy+y2)h=lim⁡h→0−4xh+2yh+h2h=lim⁡h→0(−4x+2y+h)=−4x+2y\begin{aligned} f_{y}(x, y) &=\lim _{h \rightarrow 0} \frac{f(x, y+h)-f(x, y)}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2}-4 x(y+h)+(y+h)^{2}-\left(x^{2}-4 x y+y^{2}\right)}{h} \\ &=\lim _{h \rightarrow 0} \frac{x^{2}-4 x y-4 x h+y^{2}+2 y h+h^{2}-\left(x^{2}-4 x y+y^{2}\right)}{h} \\ &=\lim _{h \rightarrow 0} \frac{-4 x h+2 y h+h^{2}}{h} \\ &=\lim _{h \rightarrow 0}(-4 x+2 y+h) \\ &=-4 x+2 y \end{aligned}

    c. f(x,y)=2x3+3xy−y2f(x, y)=2 x^{3}+3 x y-y^{2}

    Solution
    ∂f∂x=lim⁡h→0f(x+h,y)−f(x,y)h=lim⁡h→0h(6x2+6xh+2h2+3y)h=lim⁡h→0(6x2+6xh+2h2+3y)=6x2+3y∂f∂y=lim⁡h→0f(x,y+h)−f(x,y)h=lim⁡h→0h(3x−2y−h)h=lim⁡h→0(3x−2y−h)=3x−2y\begin{aligned} \frac{\partial f}{\partial x} &= \lim _{h \rightarrow 0} \frac{f(x+h, y)-f(x, y)}{h} \\ &=\lim _{h \rightarrow 0} \frac{h\left(6 x^{2}+6 x h+2 h^{2}+3 y\right)}{h} \\ &=\lim _{h \rightarrow 0}\left(6 x^{2}+6 x h+2 h^{2}+3 y\right) \\ &=6 x^{2}+3 y \\ \frac{\partial f}{\partial y} &= \lim _{h \rightarrow 0} \frac{f(x, y+h)-f(x, y)}{h} \\ &=\lim _{h \rightarrow 0} \frac{h(3 x-2 y-h)}{h} \\ &=\lim _{h \rightarrow 0}(3 x-2 y-h) \\ &=3 x-2 y \end{aligned}
  2. Determine all the first and second order partial derivatives of the function

    a. f(x,y)=x2y3+3y+xf(x, y)=x^{2} y^{3}+3 y+x

    Solution
    ∂f∂x=2xy3+1∂f∂y=3x2y2+3∂∂x(∂f∂x)=2y3∂∂y(∂f∂x)=6xy2∂∂x(∂f∂y)=6xy2∂∂y(∂f∂y)=6x2y\begin{aligned} \frac{\partial f}{\partial x}&= 2xy^3+1 \\ \frac{\partial f}{\partial y}&= 3x^2y^2+3 \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial x}\right)&= 2y^3 \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial x}\right)&= 6xy^2 \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial y}\right)&= 6xy^2 \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial y}\right)&= 6x^2y \\ \end{aligned}

    b. f(x,y)=x4sin⁡3yf(x, y)=x^{4} \sin 3 y

    Solution
    ∂f∂x=4x3sin⁡3y∂f∂y=3x4cos⁡3y∂∂x(∂f∂x)=12x2sin⁡3y∂∂y(∂f∂x)=12x3cos⁡3y∂∂x(∂f∂y)=12x3cos⁡3y∂∂y(∂f∂y)=−9x4sin⁡3y\begin{aligned} \frac{\partial f}{\partial x}&= 4x^3\sin{3y} \\ \frac{\partial f}{\partial y}&= 3x^4\cos{3y} \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial x}\right)&= 12x^2\sin{3y} \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial x}\right)&= 12x^3\cos{3y} \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial y}\right)&= 12x^3\cos{3y} \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial y}\right)&= -9x^4\sin{3y} \\ \end{aligned}

    c. f(x,y)=x2y+ln⁡(y2−x)f(x, y)=x^{2} y+\ln \left(y^{2}-x\right)

    Solution
    ∂f∂x=2xy−1y2−x∂f∂y=x2+2yy2−x∂∂x(∂f∂x)=2y−1(y2−x)2∂∂y(∂f∂x)=2x+2y(y2−x)2∂∂x(∂f∂y)=2x+2y(y2−x)2∂∂y(∂f∂y)=−2y2−2x(y2−x)2\begin{aligned} \frac{\partial f}{\partial x}&= 2xy-\frac{1}{y^2-x} \\ \frac{\partial f}{\partial y}&= x^2+\frac{2y}{y^2-x} \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial x}\right)&= 2y-\frac{1}{(y^2-x)^2} \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial x}\right)&= 2x+\frac{2y}{(y^2-x)^2} \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial y}\right)&= 2x+\frac{2y}{(y^2-x)^2} \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial y}\right)&= \frac{-2y^2-2x}{(y^2-x)^2} \\ \end{aligned}

    d. f(x,y)=exy(2x−y)f(x, y)=e^{x y}(2 x-y)

    Solution
    ∂f∂x=exy(2xy−y2+2)∂f∂y=exy(2x2−xy−1)∂∂x(∂f∂x)=exy(2xy2−y3+4y)∂∂y(∂f∂x)=exy(2x2y−xy2+4x−2y)∂∂x(∂f∂y)=exy(2x2y−xy2+4x−2y)∂∂y(∂f∂y)=exy(2x3−x2y−2x)\begin{aligned} \frac{\partial f}{\partial x}&= e^{xy}(2xy-y^2+2) \\ \frac{\partial f}{\partial y}&= e^{xy}(2x^2-xy-1) \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial x}\right)&= e^{xy}(2xy^2-y^3+4y) \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial x}\right)&= e^{xy}(2x^2y-xy^2+4x-2y) \\ \frac{\partial}{\partial x}\left(\frac{\partial f}{\partial y}\right)&= e^{xy}(2x^2y-xy^2+4x-2y) \\ \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial y}\right)&= e^{xy}(2x^3-x^2y-2x)\\ \end{aligned}
  3. Find both partial derivatives for each of the following two variables functions

    a. g(x,y)=yex+yg(x, y)=y e^{x+y}

    Solution
    g(x,y)=yex+ygx(x,y)=yex+ygy(x,y)=ex+y+yex+y\begin{aligned} g(x, y)=& y e^{x+y} \\ g_{x}(x, y) &=y e^{x+y} \\ g_{y}(x, y) &=e^{x+y}+y e^{x+y} \end{aligned}

    b. h(x,y)=xsin⁡y−ycos⁡xh(x, y)=x \sin y-y \cos x

    Solution
    h(x,y)=xsin⁡y−ycos⁡xhx(x,y)=sin⁡y+ysin⁡xhy(x,y)=xcos⁡y−cos⁡x\begin{aligned} &h(x, y)=x \sin y-y \cos x \\ &h_{x}(x, y)=\sin y+y \sin x \\ &h_{y}(x, y)=x \cos y-\cos x \end{aligned}

    c. p(x,y)=xy+y2p(x, y)=x^{y}+y^{2}

    Solution
    p(x,y)=xy+y2px(x,y)=yxy−1py(x,y)=xyln⁡x+2y\begin{aligned} p(x, y)=& x^{y}+y^{2} \\ p_{x}(x, y) &=y x^{y-1} \\ p_{y}(x, y) &=x^{y} \ln x+2 y \end{aligned}

    d. U(x,y)=9y3x−yU(x, y)=\frac{9 y^{3}}{x-y}

    Solution
    ∂U∂x=Ux=(x−y)(0)−9y3(1)(x−y)2=−9y3(x−y)2∂U∂y=Uy=(x−y)(27y2)−9y3(−1)(x−y)2=27xy2−18y3(x−y)2\begin{aligned} &\frac{\partial U}{\partial x}=U_{x}=\frac{(x-y)(0)-9 y^{3}(1)}{(x-y)^{2}}=\frac{-9 y^{3}}{(x-y)^{2}} \\ &\frac{\partial U}{\partial y}=U_{y}=\frac{(x-y)\left(27 y^{2}\right)-9 y^{3}(-1)}{(x-y)^{2}}=\frac{27 x y^{2}-18 y^{3}}{(x-y)^{2}} \end{aligned}
  4. For f(x,y,z)f(x, y, z), use the implicit function theorem to find dy/dxd y / d x and dy/dzd y / d z

    a. f(x,y,z)=x2y3+z2+xyzf(x, y, z)=x^{2} y^{3}+z^{2}+x y z

    Solution
    f(x,y,z)=x2y3+z2+xyzdydx=−fxfy=−2xy3+yz3x2y2+xzdydz=−fzfy=−2z+xy3x2y2+xz\begin{gathered} f(x, y, z)=x^{2} y^{3}+z^{2}+x y z \\ \frac{d y}{d x}=-\frac{f x}{f y}=-\frac{2 x y^{3}+y z}{3 x^{2} y^{2}+x z} \\ \frac{d y}{d z}=-\frac{f z}{f y}=-\frac{2 z+x y}{3 x^{2} y^{2}+x z} \end{gathered}

    b. f(x,y,z)=x3z2+y3+4xyzf(x, y, z)=x^{3} z^{2}+y^{3}+4 x y z

    Solution
    f(x,y,z)=x3z2+y3+4xyzdydx=−fxfy=−3x2z2+4yz3y2+4xzdydz=−fzfy=−2x3z+4xy3y2+4xz\begin{gathered} f(x, y, z)=x^{3} z^{2}+y^{3}+4 x y z \\ \frac{d y}{d x}=-\frac{f x}{f y}=-\frac{3 x^{2} z^{2}+4 y z}{3 y^{2}+4 x z} \\ \frac{d y}{d z}=-\frac{f z}{f y}=-\frac{2 x^{3} z+4 x y}{3 y^{2}+4 x z} \end{gathered}

    c. f(x,y,z)=3x2y3+xz2y2+y3zx4+y2zf(x, y, z)=3 x^{2} y^{3}+x z^{2} y^{2}+y^{3} z x^{4}+y^{2} z

    Solution
    f(x,y,z)=3x2y3+xz2y2+y3zx4+y2zdydx=−fxfy=−6xy3+z2y2+4y3zx39x2y2+2xz2y+3y2zx4+2yzdydz=−fzfy=−2xzy2+y3x4+y29x2y2+2xz2y+3y2zx4+2yz\begin{gathered} f(x, y, z)=3 x^{2} y^{3}+x z^{2} y^{2}+y^{3} z x^{4}+y^{2} z \\ \frac{d y}{d x}=-\frac{f x}{f y}=-\frac{6 x y^{3}+z^{2} y^{2}+4 y^{3} z x^{3}}{9 x^{2} y^{2}+2 x z^{2} y+3 y^{2} z x^{4}+2 y z} \\ \frac{d y}{d z}=-\frac{f z}{f y}=-\frac{2 x z y^{2}+y^{3} x^{4}+y^{2}}{9 x^{2} y^{2}+2 x z^{2} y+3 y^{2} z x^{4}+2 y z} \end{gathered}
  5. Find ∂F∂s\frac{\partial F}{\partial s} and ∂F∂t\frac{\partial F}{\partial t}, if applicable, for the following composite functions

    a. F=sin⁡(x+y)F=\sin (x+y) where x=2stx=2st and y=s2+t2y=s^2+t^2

    Solution
    ∂F∂s=∂F∂x∂x∂s+∂F∂y∂y∂s=cos⁡(x+y)(2t)+cos⁡(x+y)(2s)=2tcos⁡(2st+s2+t2)+2scos⁡(2st+s2+t2)=2cos⁡((s+t)2)(s+t)\begin{aligned} \frac{\partial F}{\partial s}&=\frac{\partial F}{\partial x}\frac{\partial x}{\partial s}+\frac{\partial F}{\partial y} \frac{\partial y}{\partial s} \\ &=\cos (x+y)(2t)+\cos (x+y)(2s) \\ &=2t\cos (2st+s^2+t^2)+2s\cos (2st+s^2+t^2) \\ &= 2\cos ((s+t)^2)(s+t) \end{aligned}∂F∂t=∂F∂x∂x∂t+∂F∂y∂y∂t=cos⁡(x+y)(2s)+cos⁡(x+y)(2t)=2cos⁡((s+t)2)(s+t)\begin{aligned} \frac{\partial F}{\partial t}&=\frac{\partial F}{\partial x}\frac{\partial x}{\partial t}+\frac{\partial F}{\partial y} \frac{\partial y}{\partial t} \\ &=\cos (x+y)(2s)+\cos (x+y)(2t) \\ &= 2\cos ((s+t)^2)(s+t) \end{aligned}

    b. F=ln⁡(x2+y)F=\ln \left(x^{2}+y\right) where x=e(s+t2)x=\mathrm{e}^{(s+t 2)} and y=s2+ty=s^{2}+t

    Solution
    ∂F∂s=∂F∂x∂x∂s+∂F∂y∂y∂s=2xx2+yes+t2+1x2+y2s=2x2+y(xes+t2+s)\begin{aligned} \frac{\partial F}{\partial s} & =\frac{\partial F}{\partial x}\frac{\partial x}{\partial s} +\frac{\partial F}{\partial y}\frac{\partial y}{\partial s}\\ & =\frac{2x}{x^{2} +y} e^{s+t^{2}} +\frac{1}{x^{2} +y} 2s\\ & =\frac{2}{x^{2} +y}\left( xe^{s+t^{2}} +s\right) \end{aligned}∂F∂t=∂F∂x∂x∂t+∂F∂y∂y∂t=2xx2+y2tes+t2+1x2+y(1)=1x2+y(4xtes+t2+1)\begin{aligned} \frac{\partial F}{\partial t} & =\frac{\partial F}{\partial x}\frac{\partial x}{\partial t} +\frac{\partial F}{\partial y}\frac{\partial y}{\partial t}\\ & =\frac{2x}{x^{2} +y} 2te^{s+t^{2}} +\frac{1}{x^{2} +y}( 1)\\ & =\frac{1}{x^{2} +y}\left( 4xte^{s+t^{2}} +1\right) \end{aligned}

    c. F=x2y2F=x^{2} y^{2} where x=scos⁡tx=s \cos t and y=ssin⁡ty=s \sin t

    Solution
    ∂F∂s=∂F∂x∂x∂s+∂F∂y∂y∂s=2xy2cos⁡t+2x2ysin⁡t=2(scos⁡t)(s2sin⁡2t)(cos⁡t)+2(s2cos⁡2t)(ssin⁡t)(sin⁡t)=2s3cos⁡2tsin⁡2t+2s3cos⁡2tsin⁡2t=4s3cos⁡2tsin⁡2t=4s3(cos⁡tsin⁡t)2=4s3(12sin⁡2t)2=s3(sin⁡2t)2\begin{aligned} \frac{\partial F}{\partial s} & =\frac{\partial F}{\partial x}\frac{\partial x}{\partial s} +\frac{\partial F}{\partial y}\frac{\partial y}{\partial s}\\ & =2xy^{2}\cos t+2x^{2} y\sin t\\ & =2( s\cos t)\left( s^{2}\sin^{2} t\right)(\cos t) +2\left( s^{2}\cos^{2} t\right)( s\sin t)(\sin t)\\ & =2s^{3}\cos^{2} t\sin^{2} t+2s^{3}\cos^{2} t\sin^{2} t\\ & =4s^{3}\cos^{2} t\sin^{2} t\\ & =4s^{3}(\cos t\sin t)^{2}\\ & =4s^{3}\left(\frac{1}{2}\sin 2t\right)^{2}\\ & =s^{3}(\sin 2t)^{2} \end{aligned}∂F∂t=∂F∂x∂x∂t+∂F∂y∂y∂t=2xy2(−ssin⁡t)+2x2y(scos⁡t)=2x2yscos⁡t−2xy2ssin⁡t=2(s2cos⁡2t)(ssin⁡t)scos⁡t−2(scos⁡t)(s2sin⁡2t)ssin⁡t=2s4cos⁡3tsin⁡t−2s4cos⁡tsin⁡3t=2s4(cos⁡tsin⁡t)(cos⁡2t−sin⁡2t)=2s4(12sin⁡2t)(cos⁡2t)=s4sin⁡2tcos⁡2t\begin{aligned} \frac{\partial F}{\partial t} & =\frac{\partial F}{\partial x}\frac{\partial x}{\partial t} +\frac{\partial F}{\partial y}\frac{\partial y}{\partial t}\\ & =2xy^{2}( -s\sin t) +2x^{2} y( s\cos t)\\ & =2x^{2} ys\cos t-2xy^{2} s\sin t\\ & =2\left( s^{2}\cos^{2} t\right)( s\sin t) s\cos t-2( s\cos t)\left( s^{2}\sin^{2} t\right) s\sin t\\ & =2s^{4}\cos^{3} t\sin t-2s^{4}\cos t\sin^{3} t\\ & =2s^{4}(\cos t\sin t)\left(\cos^{2} t-\sin^{2} t\right)\\ & =2s^{4}\left(\frac{1}{2}\sin 2t\right)(\cos 2t)\\ & =s^{4}\sin 2t\cos 2t \end{aligned}

    d. F=xy+yz2F=xy+y \mathrm{z}^{2} where x=et,y=etsin⁡tx=\mathrm{e}^{t}, y=\mathrm{e}^{t} \sin t and z=etcos⁡t\mathrm{z}=\mathrm{e}^{t} \cos t

    Solution
    dFdt=∂F∂x∂x∂t+∂F∂y∂y∂t+∂F∂z∂z∂t=yet+(x+z2)(etcos⁡t+etsin⁡t)+2yz(−etsin⁡t+etcos⁡t)=yet+xetcos⁡t+xetsin⁡t+z2etcos⁡t+z2sin⁡tet−2yzetsin⁡t+2yzetcos⁡t=yet+etcos⁡t(x+z2+2yz)+etsin⁡t(x+z2−2yz)=etsin⁡t⋅et+etcos⁡t(et+e2tcos⁡2t+2e2tsin⁡tcos⁡t)     +etsin⁡t(et+e2tcos⁡2t−2e2tsin⁡tcos⁡t)=e2tsin⁡t+e2tcos⁡t+e3tcos⁡3t+2e3tsin⁡tcos⁡2t+e2tsin⁡t+e3tsin⁡tcos⁡2t     −2e3tsin⁡2tcos⁡t=2e2tsin⁡t+e2tcos⁡t+e3tcos⁡3t+3e3tsin⁡tcos⁡2t−2e3tsin⁡2tcos⁡t=e2t(2sin⁡t+cos⁡t)+e3t(cos⁡3t+3sin⁡tcos⁡2t−2sin⁡2tcos⁡t)\begin{aligned} \frac{dF}{dt} & =\frac{\partial F}{\partial x}\frac{\partial x}{\partial t} +\frac{\partial F}{\partial y}\frac{\partial y}{\partial t} +\frac{\partial F}{\partial z}\frac{\partial z}{\partial t}\\ & =ye^{t} +\left( x+z^{2}\right)\left( e^{t}\cos t+e^{t}\sin t\right) +2yz\left( -e^{t}\sin t+e^{t}\cos t\right)\\ & =ye^{t} +xe^{t}\cos t+xe^{t}\sin t +z^{2} e^{t}\cos t+z^{2}\sin te^{t} -2yze^{t}\sin t+2yze^{t}\cos t\\ & =ye^{t} +e^{t}\cos t\left( x+z^{2} +2yz\right) +e^{t}\sin t\left( x+z^{2} -2yz\right)\\ & =e^{t}\sin t\cdot e^{t} +e^{t}\cos t\left( e^{t} +e^{2t}\cos^{2} t+2e^{2t}\sin t\cos t\right)\\ & \ \ \ \ \ +e^{t}\sin t\left( e^{t} +e^{2t}\cos^{2} t-2e^{2t}\sin t\cos t\right)\\ & =e^{2t}\sin t+e^{2t}\cos t+e^{3t}\cos^{3} t+2e^{3t}\sin t\cos^{2} t+e^{2t}\sin t+e^{3t}\sin t\cos^{2} t\\ & \ \ \ \ \ -2e^{3t}\sin^{2} t\cos t\\ & =2e^{2t}\sin t+e^{2t}\cos t+e^{3t}\cos^{3} t+3e^{3t}\sin t\cos^{2} t-2e^{3t}\sin^{2} t\cos t\\ & =e^{2t}( 2\sin t+\cos t) +e^{3t}\left(\cos^{3} t+3\sin t\cos^{2} t-2\sin^{2} t\cos t\right) \end{aligned}
  6. Find dy/dxd y / d x and dy/dzd y / d z (if applicable) for each of the following

    a. 7x2+2xy2+9y4=07 x^{2}+2 x y^{2}+9 y^{4}=0

    Solution
    dydx=−∂F∂x∂F∂y=−14x+2y236y2+4xy\begin{aligned} \frac{dy}{dx} & =-\frac{\frac{\partial F}{\partial x}}{\frac{\partial F}{\partial y}} =-\frac{14x+2y^{2}}{36y^{2} +4xy} \end{aligned}

    b. x3z2+y3+4xyz=0x^{3} z^{2}+y^{3}+4 x y z=0

    Solution
    dydx=−∂F∂x∂F∂y=−3x2z2+4yz3y2+4xzdydz=−∂F∂z∂F∂y=−2x3z+4xy3y2+4xz\begin{aligned} \frac{dy}{dx} & =-\frac{\frac{\partial F}{\partial x}}{\frac{\partial F}{\partial y}} =-\frac{3x^{2} z^{2} +4yz}{3y^{2} +4xz}\\ \frac{dy}{dz} & =-\frac{\frac{\partial F}{\partial z}}{\frac{\partial F}{\partial y}} =-\frac{2x^{3} z+4xy}{3y^{2} +4xz} \end{aligned}

    c. 3x2y3+xz2y2+y3zx4+y2z=03 x^{2} y^{3}+x z^{2} y^{2}+y^{3} z x^{4}+y^{2} z=0

    Solution
    dydx=−∂F∂x∂F∂y=−6xy3+z2y2+4y3zx39x2y2+2xz2y+3y2zx4+2yzdydz=−∂F∂z∂F∂y=−2xzy2+y3x4+y29x2y2+2xz2y+3y2zx4+2yz\begin{aligned} \frac{dy}{dx} & =-\frac{\frac{\partial F}{\partial x}}{\frac{\partial F}{\partial y}} =-\frac{6xy^{3} +z^{2} y^{2} +4y^{3} zx^{3}}{9x^{2} y^{2} +2xz^{2} y+3y^{2} zx^{4} +2yz}\\ \frac{dy}{dz} & =-\frac{\frac{\partial F}{\partial z}}{\frac{\partial F}{\partial y}} =-\frac{2xzy^{2} +y^{3} x^{4} +y^{2}}{9x^{2} y^{2} +2xz^{2} y+3y^{2} z x^{4} +2yz} \end{aligned}

    d. y5+x2y3=1+yexp⁡(x2)y^{5}+x^{2} y^{3}=1+y \exp \left(x^{2}\right)

    Solution
    dydx=−∂F∂x∂F∂y=−2xy(y2−ex2)5y4+3x2y2−ex2\begin{aligned} \frac{dy}{dx} & =-\frac{\frac{\partial F}{\partial x}}{\frac{\partial F}{\partial y}} =-\frac{2xy\left( y^{2} -e^{x^{2}}\right)}{5y^{4} +3x^{2} y^{2} -e^{x^{2}}} \end{aligned}
  7. a. In polar coordinates, x=rcos⁡θ,y=rsin⁡θx=r \cos \theta, y=r \sin \theta, show that ∂(x,y)∂(r,θ)=r\frac{\partial(x, y)}{\partial(r, \theta)}=r

    Solution
     For x=rcos⁡θ,∂x∂r=cos⁡θ,∂x∂θ=−rsin⁡θy=rsin⁡θ,∂y∂r=sin⁡θ,∂y∂θ=rcos⁡θ∴∂(x,y)∂(r,θ)=∣∂x∂r∂x∂θ∂y∂r∂y∂θ∣=∣cos⁡θ−rsin⁡θsin⁡θrcos⁡θ∣=r.\begin{aligned} & \text { For } x=r \cos \theta, \frac{\partial x}{\partial r}=\cos \theta, \frac{\partial x}{\partial \theta}=-r \sin \theta \\ & y=r \sin \theta, \frac{\partial y}{\partial r}=\sin \theta, \frac{\partial y}{\partial \theta}=r \cos \theta \\ & \therefore \quad \frac{\partial(x, y)}{\partial(r, \theta)}=\left|\begin{array}{ll}\frac{\partial x}{\partial r} & \frac{\partial x}{\partial \theta} \\\frac{\partial y}{\partial r} & \frac{\partial y}{\partial \theta}\end{array}\right|=\left|\begin{array}{cc}\cos \theta & -r \sin \theta \\\sin \theta & r \cos \theta\end{array}\right|=r . \end{aligned}

    b. Obtain the Jacobian JJ of the transformation s=2x+y,t=x−2ys=2 x+y, t=x-2 y and determine the inverse of the transformation J1J_{1}. Confirm that J1=J−1J_{1}=J^{-1}.

    Solution
    J=∂(s,t)∂(x,y)=∣211−2∣=−5\begin{aligned} J & =\frac{\partial ( s,t)}{\partial ( x,y)}\\ & =\left| \begin{matrix} 2 & 1\\ 1 & -2 \end{matrix}\right| \\ & =-5 \end{aligned}x=15(2s+t)y=15(s−2t)J1=∂(x,y)∂(s,t)=∣251515−25∣=−15\begin{array}{l} x=\frac{1}{5}( 2s+t) \quad \quad y=\frac{1}{5}( s-2t)\\ \\ \begin{aligned} J_{1} & =\frac{\partial ( x,y)}{\partial ( s,t)}\\ & =\left| \begin{matrix} \frac{2}{5} & \frac{1}{5}\\ \frac{1}{5} & -\frac{2}{5} \end{matrix}\right| \\ & =-\frac{1}{5} \end{aligned} \end{array}∴J1=J−1\therefore J_{1} =J^{-1}

    c. Show that if x+y=ux+y=\mathrm{u} and y=uvy=\mathrm{uv}, then ∂(x,y)∂(u,v)=u\frac{\partial(x, y)}{\partial(u, v)}=u.

    Solution
    x+uv=u⟹x=u−uvdxdu=1−vdxdv=−1\begin{array}{l} x+uv=u\Longrightarrow x=u-uv\\ \frac{dx}{du} =1-v\\ \frac{dx}{dv} =-1 \end{array}y=uvdydu=vdydv=u\begin{array}{l} y=uv\\ \frac{dy}{du} =v\\ \frac{dy}{dv} =u \end{array}∂(x,y)∂(u,v)=∣∂x∂u∂y∂u∂x∂v∂y∂v∣=∣1−vv−uu∣=u−uv+uv=u \begin{aligned} \frac{\partial ( x,y)}{\partial ( u,v)} & =\left| \begin{matrix} \frac{\partial x}{\partial u} & \frac{\partial y}{\partial u}\\ \frac{\partial x}{\partial v} & \frac{\partial y}{\partial v} \end{matrix}\right| \\ & =\left| \begin{matrix} 1-v & v\\ -u & u \end{matrix}\right| \\ & =u-uv+uv\\ & =u\ \end{aligned}

    d. Verify whether the functions u=x+y1−xyu=\frac{x+y}{1-x y} and v=tan⁡−1x+tan⁡−1yv=\tan ^{-1} x+\tan ^{-1} y are functionally dependent.

    Solution
    ∂(u,v)∂(x,y)=∣∂u∂x∂u∂y∂v∂x∂v∂y∣=∣1+y2(1−xy)21+x2(1−xy)211+x211+y2∣=1(1−xy)2−1(1−xy)2=0\begin{aligned} \frac{\partial ( u,v)}{\partial ( x,y)} & =\left| \begin{matrix} \frac{\partial u}{\partial x} & \frac{\partial u}{\partial y}\\ \frac{\partial v}{\partial x} & \frac{\partial v}{\partial y} \end{matrix}\right| =\left| \begin{matrix} \frac{1+y^{2}}{( 1-xy)^{2}} & \frac{1+x^{2}}{( 1-xy)^{2}}\\ \frac{1}{1+x^{2}} & \frac{1}{1+y^{2}} \end{matrix}\right| \\ & =\frac{1}{( 1-xy)^{2}} -\frac{1}{( 1-xy)^{2}}\\ & =0 \end{aligned}

    e. If x=uvx=\mathrm{uv}, y=u+vu−vy=\frac{u+v}{u-v}, find ∂(u,v)∂(x,y)\frac{\partial(u, v)}{\partial(x, y)}.

    Solution
    ∂(x,y)∂(u,v)=∣∂x∂u∂y∂u∂x∂v∂y∂v∣=∣v−2v(u−v)2u2u(u−v)2∣=2uv(u−v)2+2uv(u−v)2=4uv(u−v)2∂(u,v)∂(x,y)=(u−v)24uv\begin{aligned} \frac{\partial ( x,y)}{\partial ( u,v)} & =\left| \begin{matrix} \frac{\partial x}{\partial u} & \frac{\partial y}{\partial u}\\ \frac{\partial x}{\partial v} & \frac{\partial y}{\partial v} \end{matrix}\right| =\left| \begin{matrix} v & -\frac{2v}{( u-v)^{2}}\\ u & \frac{2u}{( u-v)^{2}} \end{matrix}\right| \\ & =\frac{2uv}{( u-v)^{2}} +\frac{2uv}{( u-v)^{2}}\\ & =\frac{4uv}{( u-v)^{2}}\\ \frac{\partial ( u,v)}{\partial ( x,y)} & =\frac{( u-v)^{2}}{4uv} \end{aligned}
  8. a. How sensitive is the volume V=πr2hV=\pi r^{2} h of a right circular cylinder to small changes in its radius and height near the point (r0,h0)=(1,3)\left(r_{0}, h_{0}\right)=(1,3)?

    Solution
    Figure for Answer 8a

    By increment method, we get

    ΔV≈(∂V∂r)(r0,h0)Δr+(∂V∂h)(r0,h0)Δh=Vr(1,3)Δr+Vh(1,3)Δh=(2πrh)(1,3)Δr+(πr2)(1,3)⋅Δh=6π⋅Δr+π⋅Δh\begin{aligned} \Delta V & \approx\left(\frac{\partial V}{\partial r}\right)_{\left(r_{0}, h_{0}\right)} \Delta r+\left(\frac{\partial V}{\partial h}\right)_{\left(r_{0}, h_{0}\right)} \Delta h \\ &=V_{r}(1,3) \Delta r+V_{h}(1,3) \Delta h \\ &=(2 \pi r h)_{(1,3)} \Delta r+\left(\pi r^{2}\right)_{(1,3)} \cdot \Delta h \\ &=6 \pi \cdot \Delta r+\pi \cdot \Delta h \end{aligned}

    The above result shows that a one-unit change in rr will change VV nearly by 6π6 \pi units and a one-unit change in hh will change VV nearly by π\pi units. Therefore, the volume of a cylinder with radius r=1r=1 and height h=3h=3 is nearly 6 times as sensitive to small change in rr as it is to small change in hh Fig. 4.3(i).

    In contrast, if the values of rr and hh are reversed, so that r=3r=3 and h=1h=1, then Vr(3,1)=2πrh=6πV_{r}(3,1)=2\pi r h=6\pi and Vh(3,1)=πr2=9πV_{h}(3,1)=\pi r^{2}=9\pi, so ΔV≈6π Δr+9π Δh\Delta V \approx 6\pi\,\Delta r+9\pi\,\Delta h. The volume is now more sensitive to a small change in hh than to a small change in rr (the rr-sensitivity is unchanged at 6π6\pi because the product rhrh is the same for both pairs; only πr2\pi r^{2} changes). Thus the sensitivity to change depends not only on the increment but also on the relative size of rr and hh (See Fig. 4.3 (ii)).

    b. If rr is measured with an accuracy of ±1%\pm 1 \% and hh with an accuracy of ±0.5%\pm 0.5 \%, about how accurately can VV be calculated from the formula V=πr2hV=\pi r^{2} h ?

    Solution

    For V=πr2hV=\pi r^{2} h or log⁡V=log⁡π+2log⁡r+log⁡h\log V=\log \pi+2 \log r+\log h, increment approximation implies

    ΔVV≈2Δrr+Δhh.\frac{\Delta V}{V} \approx 2 \frac{\Delta r}{r}+\frac{\Delta h}{h} .

    Given, Δrr×100=±1,Δhh×100=±0.5=12}\left.\quad \begin{array}{l}\frac{\Delta r}{r} \times 100=\pm 1, \\ \frac{\Delta h}{h} \times 100=\pm 0.5=\frac{1}{2}\end{array}\right\} so that ∣Δrr∣≤1100∣Δhh∣≤1200}\left.\begin{array}{l}\left|\frac{\Delta r}{r}\right| \leq \frac{1}{100} \\ \left|\frac{\Delta h}{h}\right| \leq \frac{1}{200}\end{array}\right\}

    ∴∣ΔVV∣≈∣2Δrr+Δhh∣≤2∣Δrr∣+∣Δhh∣=2100+1200=0.025\therefore\left|\frac{\Delta V}{V}\right| \approx\left|2 \frac{\Delta r}{r}+\frac{\Delta h}{h}\right| \leq 2\left|\frac{\Delta r}{r}\right|+\left|\frac{\Delta h}{h}\right|=\frac{2}{100}+\frac{1}{200}=0.025

    Thus, the maximum percentage error (or change), viz. ∣ΔVV∣×100\left|\frac{\Delta V}{V}\right| \times 100, due to possible percentage error (or change) in measurement of rr and hh will be about 2.52.5 per cent.

    c. The period TT of a simple pendulum is T=2πlgT=2 \pi \sqrt{\frac{l}{g}}, find the maximum percentage error in TT due to possible errors up to 1%1 \% in ll and 2%2 \% in gg (Hint: dll=0.01\frac{d l}{l}=0.01 and dgg=0.02\frac{d g}{g}=0.02 )

    Solution
    log⁡T=log⁡2π+12log⁡l−12log⁡gdTT=0+12ldl−12gdg=(12)(dll)−(12)(dgg)=(12)(0.01)±(12)(0.02)=0.005±0.01\begin{aligned} \log T & =\log 2\pi +\frac{1}{2}\log l-\frac{1}{2}\log g\\ \frac{dT}{T} & =0+\frac{1}{2l} dl-\frac{1}{2g} dg\\ & =\left(\frac{1}{2}\right)\left(\frac{dl}{l}\right) -\left(\frac{1}{2}\right)\left(\frac{dg}{g}\right)\\ & =\left(\frac{1}{2}\right)( 0.01) \pm \left(\frac{1}{2}\right)( 0.02)\\ & =0.005\pm 0.01 \end{aligned}∴Max error= 1.5%\therefore \text{Max error} =\ 1.5\%

    d. The range RR of a projectile which starts with a velocity vv at an elevation α\alpha is given by R=R= v2sin⁡2αg\frac{v^{2} \sin 2 \alpha}{g}. Find the percentage error in RR due to an error of 1%1 \% in v\mathrm{v} and an error of 0.5%0.5 \% in α\alpha.

    Solution

    Given R=v2sin⁡2αgR=\frac{v^{2} \sin 2 \alpha}{g} or log⁡R=2log⁡v+log⁡sin⁡2α−log⁡g\log R=2 \log v+\log \sin 2 \alpha-\log g.

    By error approximation (i.e. taking differential on both sides)

    δRR=2δvv+1sin⁡2αcos⁡2α⋅2δα,(δg=0)\frac{\delta R}{R}=2 \frac{\delta v}{v}+\frac{1}{\sin 2 \alpha} \cos 2 \alpha \cdot 2 \delta \alpha,(\delta g=0)

    or

    (δRR×100)=2(δvv×100)+2α(cot⁡2α)(δαα×100)=2×1+2α⋅cot⁡2α×0.5=2+2αcot⁡2α×12=(2+αcot⁡2α)\begin{aligned} \left(\frac{\delta R}{R} \times 100\right) &=2\left(\frac{\delta v}{v} \times 100\right)+2 \alpha(\cot 2 \alpha)\left(\frac{\delta \alpha}{\alpha} \times 100\right) \\ &=2 \times 1+2 \alpha \cdot \cot 2 \alpha \times 0.5=2+2 \alpha \cot 2 \alpha \times \frac{1}{2} \\ &=(2+\alpha \cot 2 \alpha) \end{aligned}

    Hence, the percentage error in calculation of RR due to errors of 1%1 \% in RR and 0.5%0.5 \% in α\alpha is (2+αcot⁡2α)(2+\alpha \cot 2 \alpha).

  9. Find the equations of the tangent plane and normal line to the following surfaces at the points indicated:

    a. x2+2y2+3z2=6x^{2}+2 y^{2}+3 z^{2}=6 at (1,1,1)(1,1,1)

    Solution

    Partial derivation yields:

    ∂f∂x=2x∂f∂y=4y∂f∂z=6z\frac{\partial f}{\partial x} =2x\quad \quad \frac{\partial f}{\partial y} =4y\quad \quad \frac{\partial f}{\partial z} =6z

    ⟹ ∂f∂x(1,1,1)=2∂f∂y(1,1,1)=4∂f∂z(1,1,1)=6\Longrightarrow \ \frac{\partial f}{\partial x}_{( 1,1,1)} =2\quad \quad \frac{\partial f}{\partial y}_{( 1,1,1)} =4\quad \quad \frac{\partial f}{\partial z}_{( 1,1,1)} =6

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=02(x−1)+4(y−1)+6(z−1)=02x−2+4y−4+6z−6=0x+2y+3z=6\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ 2( x-1) +4( y-1) +6( z-1) & =0\\ 2x-2+4y-4+6z-6 & =0\\ x+2y+3z & =6 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−12=y−14=z−16x−11=y−12=z−13\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-1}{2} & =\frac{y-1}{4} =\frac{z-1}{6}\\ \frac{x-1}{1} & =\frac{y-1}{2} =\frac{z-1}{3} \end{aligned}

    b. 2x2+y2−z2=−32 x^{2}+y^{2}-z^{2}=-3 at (1,2,3)(1,2,3)

    Solution

    Partial derivation yields:

    ∂f∂x=4x∂f∂y=2y∂f∂z=−2z\frac{\partial f}{\partial x} =4x\quad \quad \frac{\partial f}{\partial y} =2y\quad \quad \frac{\partial f}{\partial z} =-2z

    ⟹ ∂f∂x(1,2,3)=4∂f∂y(1,2,3)=4∂f∂z(1,2,3)=−6\Longrightarrow \ \frac{\partial f}{\partial x}_{( 1,2,3)} =4\quad \quad \frac{\partial f}{\partial y}_{( 1,2,3)} =4\quad \quad \frac{\partial f}{\partial z}_{( 1,2,3)} =-6

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=04(x−1)+4(y−2)−6(z−3)=04x−4+4y−8−6z+18=04x+4y−6z=−62x+2y−3z=−3\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ 4( x-1) +4( y-2) -6( z-3) & =0\\ 4x-4+4y-8-6z+18 & =0\\ 4x+4y-6z & =-6\\ 2x+2y-3z & =-3 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−14=y−24=z−3−6x−12=y−22=z−3−3\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-1}{4} & =\frac{y-2}{4} =\frac{z-3}{-6}\\ \frac{x-1}{2} & =\frac{y-2}{2} =\frac{z-3}{-3} \end{aligned}

    c. x2+y2−z=1x^{2}+y^{2}-z=1 at (1,2,4)(1,2,4)

    Solution

    Partial derivation yields:

    ∂f∂x=2x∂f∂y=2y∂f∂z=−1\frac{\partial f}{\partial x} =2x\quad \quad \frac{\partial f}{\partial y} =2y\quad \quad \frac{\partial f}{\partial z} =-1

    ⟹ ∂f∂x(1,2,4)=2∂f∂y(1,2,4)=4∂f∂z(1,2,4)=−1\Longrightarrow \ \frac{\partial f}{\partial x}_{( 1,2,4)} =2\quad \quad \frac{\partial f}{\partial y}_{( 1,2,4)} =4\quad \quad \frac{\partial f}{\partial z}_{( 1,2,4)} =-1

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=02(x−1)+4(y−2)−1(z−4)=02x−2+4y−8−z+4=02x+4y−z=6\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ 2( x-1) +4( y-2) -1( z-4) & =0\\ 2x-2+4y-8-z+4 & =0\\ 2x+4y-z & =6 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−12=y−24=z−4−1\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-1}{2} & =\frac{y-2}{4} =\frac{z-4}{-1} \end{aligned}

    d. ln⁡(xy)−z2(x−2y)−3z=3\displaystyle \ln \left(\frac{x}{y}\right)-z^{2}(x-2 y)-3 z=3 at (4,2,−1)(4,2,-1)

    Solution

    Partial derivation yields:

    ∂f∂x=1x−z2∂f∂y=2z2−1y∂f∂z=−2z(x−2y)−3\frac{\partial f}{\partial x} =\frac{1}{x} -z^{2} \quad \quad \frac{\partial f}{\partial y} =2z^{2} -\frac{1}{y} \quad \quad \frac{\partial f}{\partial z} =-2z( x-2y) -3

    ⟹ ∂f∂x(4,2,−1)=−34∂f∂y(4,2,−1)=32∂f∂z(4,2,−1)=−3\Longrightarrow \ \frac{\partial f}{\partial x}_{( 4,2,-1)} =-\frac{3}{4} \quad \quad \frac{\partial f}{\partial y}_{( 4,2,-1)} =\frac{3}{2} \quad \quad \frac{\partial f}{\partial z}_{( 4,2,-1)} =-3

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=0−34(x−4)+32(y−2)−3(z+1)=0−34x+3+32y−3−3z−3=0−34x+32y−3z=3\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ -\frac{3}{4}( x-4) +\frac{3}{2}( y-2) -3( z+1) & =0\\ -\frac{3}{4} x+3+\frac{3}{2} y-3-3z-3 & =0\\ -\frac{3}{4} x+\frac{3}{2} y-3z & =3 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−4−34=y−232=z+1−3\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-4}{-\frac{3}{4}} & =\frac{y-2}{\frac{3}{2}} =\frac{z+1}{-3} \end{aligned}

    e. x3z+z3x−2yz=0x^{3} z+z^{3} x-2 y z=0 at (1,1,1)(1,1,1)

    Solution

    Partial derivation yields:

    ∂f∂x=3x2z+z3∂f∂y=−2z∂f∂z=x3+3z2x−2y\frac{\partial f}{\partial x} =3x^{2} z+z^{3} \quad \quad \frac{\partial f}{\partial y} =-2z\quad \quad \frac{\partial f}{\partial z} =x^{3} +3z^{2} x-2y

    ⟹ ∂f∂x(1,1,1)=4∂f∂y(1,1,1)=−2∂f∂z(1,1,1)=2\Longrightarrow \ \frac{\partial f}{\partial x}_{( 1,1,1)} =4\quad \quad \frac{\partial f}{\partial y}_{( 1,1,1)} =-2\quad \quad \frac{\partial f}{\partial z}_{( 1,1,1)} =2

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=04(x−1)−2(y−1)+2(z−1)=04x−4−2y+2+2z−2=04x−2y+2z=42x−y+z=2\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ 4( x-1) -2( y-1) +2( z-1) & =0\\ 4x-4-2y+2+2z-2 & =0\\ 4x-2y+2z & =4\\ 2x-y+z & =2 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−14=y−1−2=z−12x−12=y−1−1=z−11\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-1}{4} & =\frac{y-1}{-2} =\frac{z-1}{2}\\ \frac{x-1}{2} & =\frac{y-1}{-1} =\frac{z-1}{1} \end{aligned}

    f. z=5+(x−1)2+(y+2)2z=5+(x-1)^{2}+(y+2)^{2} at (2,0,10)(2,0,10)

    Solution

    z=5+(x−1)2+(y+2)2⟹(x−1)2+(y+2)2−z=−5z=5+( x-1)^{2} +( y+2)^{2} \Longrightarrow ( x-1)^{2} +( y+2)^{2} -z=-5

    Partial derivation yields:

    ∂f∂x=2(x−1)∂f∂y=2(y+2)∂f∂z=−1\frac{\partial f}{\partial x} =2( x-1) \quad \quad \frac{\partial f}{\partial y} =2( y+2) \quad \quad \frac{\partial f}{\partial z} =-1

    ⟹ ∂f∂x(2,0,10)=2∂f∂y(2,0,10)=4∂f∂z(2,0,10)=−1\Longrightarrow \ \frac{\partial f}{\partial x}_{( 2,0,10)} =2\quad \quad \frac{\partial f}{\partial y}_{( 2,0,10)} =4\quad \quad \frac{\partial f}{\partial z}_{( 2,0,10)} =-1

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=02(x−2)+4(y)−(z−10)=02x−4+4y−z+10=02x+4y−z=−6\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ 2( x-2) +4( y) -( z-10) & =0\\ 2x-4+4y-z+10 & =0\\ 2x+4y-z & =-6 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−22=y4=z−10−1\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-2}{2} & =\frac{y}{4} =\frac{z-10}{-1} \end{aligned}

    g. x212+y26+z24=1\displaystyle\frac{x^{2}}{12}+\frac{y^{2}}{6}+\frac{z^{2}}{4}=1 at (1,2,1)(1,2,1)

    Solution

    Partial derivation yields:

    ∂f∂x=x6∂f∂y=y3∂f∂z=z2\frac{\partial f}{\partial x} =\frac{x}{6} \quad \quad \frac{\partial f}{\partial y} =\frac{y}{3} \quad \quad \frac{\partial f}{\partial z} =\frac{z}{2}

    ⟹ ∂f∂x(1,2,1)=16∂f∂y(1,2,1)=23∂f∂z(1,2,1)=12\Longrightarrow \ \frac{\partial f}{\partial x}_{( 1,2,1)} =\frac{1}{6} \quad \quad \frac{\partial f}{\partial y}_{( 1,2,1)} =\frac{2}{3} \quad \quad \frac{\partial f}{\partial z}_{( 1,2,1)} =\frac{1}{2}

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=016(x−1)+23(y−2)+12(z−1)=016x−16+23y−43+12z−12=016x+46y+36z−16−86−36=016x+46y+36z−2=0x+4y+3z=12\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ \frac{1}{6}( x-1) +\frac{2}{3}( y-2) +\frac{1}{2}( z-1) & =0\\ \frac{1}{6} x-\frac{1}{6} +\frac{2}{3} y-\frac{4}{3} +\frac{1}{2} z-\frac{1}{2} & =0\\ \frac{1}{6} x+\frac{4}{6} y+\frac{3}{6} z-\frac{1}{6} -\frac{8}{6} -\frac{3}{6} & =0\\ \frac{1}{6} x+\frac{4}{6} y+\frac{3}{6} z-2 & =0\\ x+4y+3z & =12 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x−116=y−223=z−112x−116=y−246=z−136x−11=y−24=z−13\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x-1}{\frac{1}{6}} & =\frac{y-2}{\frac{2}{3}} =\frac{z-1}{\frac{1}{2}}\\ \frac{x-1}{\frac{1}{6}} & =\frac{y-2}{\frac{4}{6}} =\frac{z-1}{\frac{3}{6}}\\ \frac{x-1}{1} & =\frac{y-2}{4} =\frac{z-1}{3} \end{aligned}

    h. zex+ez+1+xy+y=3z e^{x}+e^{z+1}+x y+y=3 at (0,3,−1)(0,3,-1)

    Solution

    Partial derivation yields:

    ∂f∂x=zex+y∂f∂y=x+1∂f∂z=ex+ez+1\frac{\partial f}{\partial x} =ze^{x} +y\quad \quad \frac{\partial f}{\partial y} =x+1\quad \quad \frac{\partial f}{\partial z} =e^{x} +e^{z+1}

    ⟹ ∂f∂x(0,3,−1)=2∂f∂y(0,3,−1)=1∂f∂z(0,3,−1)=2\Longrightarrow \ \frac{\partial f}{\partial x}_{( 0,3,-1)} =2\quad \quad \frac{\partial f}{\partial y}_{( 0,3,-1)} =1\quad \quad \frac{\partial f}{\partial z}_{( 0,3,-1)} =2

    Tangent plane:

    (x−xo)(∂f∂x)0+(y−y0)(∂f∂y)0+(z−z0)(∂f∂z)0=02(x)+(y−3)+2(z+1)=02x+y−3+2z+2=02x+y+2z=1\begin{aligned} ( x-x_{o})\left(\frac{\partial f}{\partial x}\right)_{0} +( y-y_{0})\left(\frac{\partial f}{\partial y}\right)_{0} +( z-z_{0})\left(\frac{\partial f}{\partial z}\right)_{0} & =0\\ 2( x) +( y-3) +2( z+1) & =0\\ 2x+y-3+2z+2 & =0\\ 2x+y+2z & =1 \end{aligned}

    Normal line:

    x−x0(∂f∂x)0=y−y0(∂f∂y)0=z−z0(∂f∂z)0x2=y−31=z+12\begin{aligned} \frac{x-x_{0}}{\left(\frac{\partial f}{\partial x}\right)_{0}} & =\frac{y-y_{0}}{\left(\frac{\partial f}{\partial y}\right)_{0}} =\frac{z-z_{0}}{\left(\frac{\partial f}{\partial z}\right)_{0}}\\ \frac{x}{2} & =\frac{y-3}{1} =\frac{z+1}{2} \end{aligned}