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Evaluate the surface integral of vector A over the plane x+y+z=1 in the first octant. Using spherical coordinates, evaluate the integral of (x²+y²+z²)dxdydz where V is the sphere x²+y²+z²=a² in the first octant.

Physics

ScanSolve AI Answer

Answer

ii

Φ(t)=[cosh⁡5t−sinh⁡5t−sinh⁡5tcosh⁡5t]\Phi(t)=\begin{bmatrix}\cosh5t&-\sinh5t\\-\sinh5t&\cosh5t\end{bmatrix}

40103\dfrac{40\sqrt{10}}{3}

Step-by-step solution

7 steps

Triple integral using spherical coordinates

Step 1: The region is x2+y2+z2≤4x^2 + y^2 + z^2 \leq 4, x≥0x \geq 0, y≥0y \geq 0, z≥0z \geq 0. In spherical coordinates, 0≤ρ≤20 \leq \rho \leq 2, 0≤θ≤π/20 \leq \theta \leq \pi/2, 0≤ϕ≤π/20 \leq \phi \leq \pi/2. Integrand (x2+y2+z2)3/4=ρ3/2(x^2 + y^2 + z^2)^{3/4} = \rho^{3/2}. dV=ρ2sin⁡ϕ dρ dϕ dθdV = \rho^2 \sin\phi \, d\rho \, d\phi \, d\theta.

I=∫0π/2∫0π/2∫02ρ3/2ρ2sin⁡ϕ dρ dϕ dθ=∫0π/2∫0π/2∫02ρ7/2sin⁡ϕ dρ dϕ dθ.I = \int_0^{\pi/2} \int_0^{\pi/2} \int_0^2 \rho^{3/2} \rho^2 \sin\phi \, d\rho \, d\phi \, d\theta = \int_0^{\pi/2} \int_0^{\pi/2} \int_0^2 \rho^{7/2} \sin\phi \, d\rho \, d\phi \, d\theta.

Step 2: ∫02ρ7/2 dρ=[29ρ9/2]02=29⋅29/2=29⋅24+1/2=29⋅162=3229\int_0^2 \rho^{7/2} \, d\rho = \left[ \frac{2}{9} \rho^{9/2} \right]_0^2 = \frac{2}{9} \cdot 2^{9/2} = \frac{2}{9} \cdot 2^{4 + 1/2} = \frac{2}{9} \cdot 16\sqrt{2} = \frac{32\sqrt{2}}{9}.

Step 3: ∫0π/2sin⁡ϕ dϕ=[−cos⁡ϕ]0π/2=1\int_0^{\pi/2} \sin\phi \, d\phi = [-\cos\phi]_0^{\pi/2} = 1.

Step 4: ∫0π/2dθ=π/2\int_0^{\pi/2} d\theta = \pi/2.

Step 5: I=3229⋅1⋅π2=16π29I = \frac{32\sqrt{2}}{9} \cdot 1 \cdot \frac{\pi}{2} = \frac{16\pi\sqrt{2}}{9}.

\dfrac{16\pi\sqrt{2}}{9}

Eigenvalues of A=[121−112]A = \begin{bmatrix} \frac{1}{2} & 1 \\ -1 & \frac{1}{2} \end{bmatrix}

Step 1: A−λI=[12−λ1−112−λ]A - \lambda I = \begin{bmatrix} \frac{1}{2}-\lambda & 1 \\ -1 & \frac{1}{2}-\lambda \end{bmatrix}.

det⁡(A−λI)=(12−λ)2−(1)(−1)=(12−λ)2+1=0\det(A - \lambda I) = \left(\frac{1}{2} - \lambda\right)^2 - (1)(-1) = \left(\frac{1}{2} - \lambda\right)^2 + 1 = 0.

Step 2: (12−λ)2=−1\left(\frac{1}{2} - \lambda\right)^2 = -1, 12−λ=±i\frac{1}{2} - \lambda = \pm i, λ=12∓i\lambda = \frac{1}{2} \mp i.

\lambda = \dfrac{1}{2} \pm i

Linear system dxdt=−5y\frac{dx}{dt} = -5y, dydt=−5x\frac{dy}{dt} = -5x

Part i

Step 1: Let X(t)=[xy]\mathbf{X}(t) = \begin{bmatrix} x \\ y \end{bmatrix}. Then dXdt=[0−5−50]X\frac{d\mathbf{X}}{dt} = \begin{bmatrix} 0 & -5 \\ -5 & 0 \end{bmatrix} \mathbf{X}.

Part ii

Φ(t)=[cosh⁡5t−sinh⁡5t−sinh⁡5tcosh⁡5t]\Phi(t)=\begin{bmatrix}\cosh5t&-\sinh5t\\-\sinh5t&\cosh5t\end{bmatrix}

Step 1: A=[0−5−50]A = \begin{bmatrix} 0 & -5 \\ -5 & 0 \end{bmatrix}. Characteristic equation: det⁡(A−λI)=λ2−25=0\det(A - \lambda I) = \lambda^2 - 25 = 0, λ=±5\lambda = \pm 5.

  1. For λ=5\lambda=5, (A−5I)v=0(A - 5I)\mathbf{v} = 0 gives v1=[1−1]\mathbf{v}_1 = \begin{bmatrix} 1 \\ -1 \end{bmatrix}.

    For λ=−5\lambda=-5, v2=[11]\mathbf{v}_2 = \begin{bmatrix} 1 \\ 1 \end{bmatrix}.

  2. P=[11−11]P = \begin{bmatrix} 1 & 1 \\ -1 & 1 \end{bmatrix}, det⁡P=2\det P = 2, P−1=12[1−111]P^{-1} = \frac{1}{2} \begin{bmatrix} 1 & -1 \\ 1 & 1 \end{bmatrix}.

  3. Φ(t)=P[e5t00e−5t]P−1=[cosh⁡(5t)−sinh⁡(5t)−sinh⁡(5t)cosh⁡(5t)]\Phi(t) = P \begin{bmatrix} e^{5t} & 0 \\ 0 & e^{-5t} \end{bmatrix} P^{-1} = \begin{bmatrix} \cosh(5t) & -\sinh(5t) \\ -\sinh(5t) & \cosh(5t) \end{bmatrix}.

    \Phi(t)=\begin{bmatrix}\cosh5t&-\sinh5t\-\sinh5t&\cosh5t\end{bmatrix}

    Green's theorem: ∮C(x−y) dx+(x+y) dy\oint_C (x-y)\,dx + (x+y)\,dy, CC bounds x=0x=0, y=0y=0, y=10−x2y=10-x^2

  4. P=x−yP=x-y, Q=x+yQ=x+y.

    ∂Q∂x−∂P∂y=1−(−1)=2\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 1 - (-1) = 2.

  5. ∮C=∬D2 dA=2⋅Area(D)\oint_C = \iint_D 2\, dA = 2 \cdot \text{Area}(D).

  6. DD

    0≤x≤100 \leq x \leq \sqrt{10}, 0≤y≤10−x20 \leq y \leq 10-x^2.

    Area = ∫010(10−x2) dx=[10x−x33]010=1010−103/23=1010(1−13)=20103\int_0^{\sqrt{10}} (10 - x^2)\, dx = \left[10x - \frac{x^3}{3}\right]_0^{\sqrt{10}} = 10\sqrt{10} - \frac{10^{3/2}}{3} = 10\sqrt{10} \left(1 - \frac{1}{3}\right) = \frac{20\sqrt{10}}{3}.

  7. ∮C=2⋅20103=40103\oint_C = 2 \cdot \frac{20\sqrt{10}}{3} = \frac{40\sqrt{10}}{3}.

    \dfrac{40\sqrt{10}}{3}

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