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Evaluate A · n d S, where A=(x+y) i+(y+z) j+x y z k and S is the surface of the plane x+y+z=1 in the first octant.

Mathematics

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Step-by-step solution

16 steps

Part a· 5 steps

  1. The surface SS is ϕ=π/4\phi = \pi/4, 0≤ρ≤10 \leq \rho \leq 1, 0≤θ≤π/20 \leq \theta \leq \pi/2 (portion of cone inside unit sphere, first octant).

    r(ρ,θ)=(ρsin⁡ϕcos⁡θ,ρsin⁡ϕsin⁡θ,ρcos⁡ϕ),ϕ=π/4.\mathbf{r}(\rho, \theta) = (\rho \sin\phi \cos\theta, \rho \sin\phi \sin\theta, \rho \cos\phi), \quad \phi = \pi/4.

    Surface element: dS=ρsin⁡ϕ dρ dθdS = \rho \sin\phi \, d\rho \, d\theta.

  2. x−y=ρsin⁡ϕ(cos⁡θ−sin⁡θ)x - y = \rho \sin\phi (\cos\theta - \sin\theta).

    ∬S(x−y) dS=∫0π/2∫01ρsin⁡ϕ(cos⁡θ−sin⁡θ)⋅ρsin⁡ϕ dρ dθ=sin⁡2ϕ∫0π/2(cos⁡θ−sin⁡θ) dθ∫01ρ2 dρ.\iint_S (x - y) \, dS = \int_0^{\pi/2} \int_0^1 \rho \sin\phi (\cos\theta - \sin\theta) \cdot \rho \sin\phi \, d\rho \, d\theta = \sin^2\phi \int_0^{\pi/2} (\cos\theta - \sin\theta) \, d\theta \int_0^1 \rho^2 \, d\rho.
  3. sin⁡(π/4)=22\sin(\pi/4) = \frac{\sqrt{2}}{2}, so sin⁡2ϕ=12\sin^2\phi = \frac{1}{2}.

    ∫01ρ2 dρ=[ρ33]01=13.\int_0^1 \rho^2 \, d\rho = \left[ \frac{\rho^3}{3} \right]_0^1 = \frac{1}{3}.
  4. ∫0π/2cos⁡θ dθ=[sin⁡θ]0π/2=1−0=1\int_0^{\pi/2} \cos\theta \, d\theta = \left[ \sin\theta \right]_0^{\pi/2} = 1 - 0 = 1,

    ∫0π/2sin⁡θ dθ=[−cos⁡θ]0π/2=0−(−1)=1\int_0^{\pi/2} \sin\theta \, d\theta = \left[ -\cos\theta \right]_0^{\pi/2} = 0 - (-1) = 1,

    so ∫0π/2(cos⁡θ−sin⁡θ) dθ=1−1=0\int_0^{\pi/2} (\cos\theta - \sin\theta) \, d\theta = 1 - 1 = 0.

  5. Integral =12⋅0⋅13=0= \frac{1}{2} \cdot 0 \cdot \frac{1}{3} = \boxed{0}.

Part b· 4 steps

  1. x2+y2=ρsin⁡ϕ\sqrt{x^2 + y^2} = \rho \sin\phi, dV=ρ2sin⁡ϕ dρ dϕ dθdV = \rho^2 \sin\phi \, d\rho \, d\phi \, d\theta.

    Region VV: 0≤θ≤π/20 \leq \theta \leq \pi/2, 0≤ϕ≤π/40 \leq \phi \leq \pi/4, 0≤ρ≤10 \leq \rho \leq 1.

    ∭Vx2+y2 dV=∫0π/2dθ∫0π/4sin⁡2ϕ dϕ∫01ρ3 dρ.\iiint_V \sqrt{x^2 + y^2} \, dV = \int_0^{\pi/2} d\theta \int_0^{\pi/4} \sin^2\phi \, d\phi \int_0^1 \rho^3 \, d\rho.
  2. ∫0π/2dθ=π/2\int_0^{\pi/2} d\theta = \pi/2,

    ∫01ρ3 dρ=[ρ44]01=1/4\int_0^1 \rho^3 \, d\rho = \left[ \frac{\rho^4}{4} \right]_0^1 = 1/4.

  3. sin⁡2ϕ=1−cos⁡2ϕ2\sin^2\phi = \frac{1 - \cos 2\phi}{2},

    ∫0π/4sin⁡2ϕ dϕ=∫0π/41−cos⁡2ϕ2 dϕ=12[ϕ−sin⁡2ϕ2]0π/4=12(π4−sin⁡(π/2)2)=12(π4−12)=π8−14.\int_0^{\pi/4} \sin^2\phi \, d\phi = \int_0^{\pi/4} \frac{1 - \cos 2\phi}{2} \, d\phi = \frac{1}{2} \left[ \phi - \frac{\sin 2\phi}{2} \right]_0^{\pi/4} = \frac{1}{2} \left( \frac{\pi}{4} - \frac{\sin(\pi/2)}{2} \right) = \frac{1}{2} \left( \frac{\pi}{4} - \frac{1}{2} \right) = \frac{\pi}{8} - \frac{1}{4}.
  4. Total =π2⋅(π8−14)⋅14=π8(π8−14)=π264−π32=π264−π32= \frac{\pi}{2} \cdot \left( \frac{\pi}{8} - \frac{1}{4} \right) \cdot \frac{1}{4} = \frac{\pi}{8} \left( \frac{\pi}{8} - \frac{1}{4} \right) = \frac{\pi^2}{64} - \frac{\pi}{32} = \boxed{\dfrac{\pi^2}{64} - \dfrac{\pi}{32}}.

Part c· 2 steps

  1. A=[1001]A = \begin{bmatrix} 1 & 0 \\ 0 & 1 \end{bmatrix}.

    Characteristic equation: det⁡(A−λI)=(1−λ)2=0\det(A - \lambda I) = (1 - \lambda)^2 = 0, so λ=1\lambda = 1 (multiplicity 2).

  2. Eigenvectors

    (A−I)v=0(A - I)\mathbf{v} = \mathbf{0} gives zero matrix equation, eigenspace is all R2\mathbb{R}^2.

    Basis: v1=[10]\mathbf{v}_1 = \begin{bmatrix} 1 \\ 0 \end{bmatrix}, v2=[01]\mathbf{v}_2 = \begin{bmatrix} 0 \\ 1 \end{bmatrix}.

    \lambda=1 (mult. 2),\ eigenspace\ \mathbb{R}^2

Part d· 2 steps

  1. V=[−1001]V = \begin{bmatrix} -1 & 0 \\ 0 & 1 \end{bmatrix}.

    det⁡(V−λI)=(−1−λ)(1−λ)=0\det(V - \lambda I) = (-1 - \lambda)(1 - \lambda) = 0, so λ1=−1\lambda_1 = -1, λ2=1\lambda_2 = 1.

  2. For λ1=−1\lambda_1 = -1

    (V+I)v=[0002]v=0(V + I)\mathbf{v} = \begin{bmatrix} 0 & 0 \\ 0 & 2 \end{bmatrix} \mathbf{v} = \mathbf{0}, so v1=[10]\mathbf{v}_1 = \begin{bmatrix} 1 \\ 0 \end{bmatrix}.

    For λ2=1\lambda_2 = 1: (V−I)v=[−2000]v=0(V - I)\mathbf{v} = \begin{bmatrix} -2 & 0 \\ 0 & 0 \end{bmatrix} \mathbf{v} = \mathbf{0}, so v2=[01]\mathbf{v}_2 = \begin{bmatrix} 0 \\ 1 \end{bmatrix}.

    \lambda_1=-1\ ( \begin{bmatrix} 1 \ 0 \end{bmatrix} ),\ \lambda_2=1\ ( \begin{bmatrix} 0 \ 1 \end{bmatrix} )

Part e

System dxdt=x2−y2\dfrac{dx}{dt} = x^2 - y^2, dydt=−y2\dfrac{dy}{dt} = -y^2 in vector form

ddt[xy]=[x2−y2−y2].\dfrac{d}{dt} \begin{bmatrix} x \\ y \end{bmatrix} = \begin{bmatrix} x^2 - y^2 \\ -y^2 \end{bmatrix}.

\dot{x} = \begin{bmatrix} x^{2}-y^{2} \ -y^{2} \end{bmatrix}

Part f· 1 step

Assuming linear system x˙=Vx\dot{\mathbf{x}} = V \mathbf{x} with VV from (d).

Fundamental matrix (transition) Φ(t)=eVt=[e−t00et]\Phi(t) = e^{V t} = \begin{bmatrix} e^{-t} & 0 \\ 0 & e^{t} \end{bmatrix} (diagonal).

  1. Since VV diagonal, eVt=[e−t00et]e^{V t} = \begin{bmatrix} e^{-t} & 0 \\ 0 & e^{t} \end{bmatrix}.

    \Phi(t)=\begin{bmatrix} e^{-t} & 0 \ 0 & e^{t} \end{bmatrix}

Part g

Solution x(t)=Φ(t)x(0)\mathbf{x}(t) = \Phi(t) \mathbf{x}(0).

x(t)=[e−t00et][x(0)y(0)]=[x(0)e−ty(0)et].\mathbf{x}(t) = \begin{bmatrix} e^{-t} & 0 \\ 0 & e^{t} \end{bmatrix} \begin{bmatrix} x(0) \\ y(0) \end{bmatrix} = \begin{bmatrix} x(0) e^{-t} \\ y(0) e^{t} \end{bmatrix}.

\begin{bmatrix} x(t) \ y(t) \end{bmatrix} = \begin{bmatrix} x(0)e^{-t} \ y(0)e^{t} \end{bmatrix}

Part h· 2 steps

Green's theorem for ∮CP dx+Q dy\oint_C P\,dx + Q\,dy, P=x2−y2P = x^2 - y^2, Q=x2+y2Q = x^2 + y^2, CC: upper semicircle x2+y2=1x^2 + y^2 = 1, y≥0y \geq 0 + x-axis from (1,0) to (-1,0) (counterclockwise).

∬R(∂Q∂x−∂P∂y)dA=∬R(2x−(−2y)) dA=∬R2(x+y) dA,\iint_R \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) dA = \iint_R (2x - (-2y)) \, dA = \iint_R 2(x + y) \, dA,

RR: x2+y2≤1x^2 + y^2 \leq 1, y≥0y \geq 0.

  1. Polar

    x=rcos⁡θx = r \cos\theta, y=rsin⁡θy = r \sin\theta, dA=r dr dθdA = r \, dr \, d\theta, θ:0→π\theta: 0 \to \pi, r:0→1r: 0 \to 1.

    2∫0π∫01(rcos⁡θ+rsin⁡θ)r dr dθ=2∫0π(cos⁡θ+sin⁡θ)dθ∫01r2 dr.2 \int_0^\pi \int_0^1 (r \cos\theta + r \sin\theta) r \, dr \, d\theta = 2 \int_0^\pi (\cos\theta + \sin\theta) d\theta \int_0^1 r^2 \, dr.
  2. ∫01r2 dr=1/3\int_0^1 r^2 \, dr = 1/3,

    ∫0πcos⁡θ dθ=[sin⁡θ]0π=0\int_0^\pi \cos\theta \, d\theta = [\sin\theta]_0^\pi = 0,

    ∫0πsin⁡θ dθ=[−cos⁡θ]0π=1−(−1)=2\int_0^\pi \sin\theta \, d\theta = [-\cos\theta]_0^\pi = 1 - (-1) = 2,

    so 2⋅(0+2)⋅13=2⋅2⋅13=432 \cdot (0 + 2) \cdot \frac{1}{3} = 2 \cdot 2 \cdot \frac{1}{3} = \frac{4}{3}.

    \dfrac{4}{3}

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