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Show that any function given by omega = (ax)(by)e^-sqrt(a2+b2)z satisfies Laplace's equation in three dimensions. (d2 omega)/(d x2) + (d2 omega)/(d y2) + (d2 omega)/(d z2) = 0

Mathematics

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here is the answer to question 2a:

2a. Show that any function given by ω=sin⁡(ax)cos⁡(by)e−a2+b2z\omega = \sin(ax)\cos(by)e^{-\sqrt{a^2+b^2}z} satisfies Laplace's equation in three dimensions: ∂2ω∂x2+∂2ω∂y2+∂2ω∂z2=0\frac{\partial^2 \omega}{\partial x^2} + \frac{\partial^2 \omega}{\partial y^2} + \frac{\partial^2 \omega}{\partial z^2} = 0.

  1. Calculate the first and second partial derivatives of ω\omega with respect to xx.

    Let Cy=cos⁡(by)C_y = \cos(by) and Ez=e−a2+b2zE_z = e^{-\sqrt{a^2+b^2}z}. Then ω=sin⁡(ax)CyEz\omega = \sin(ax) C_y E_z.

    ∂ω∂x=acos⁡(ax)CyEz\frac{\partial \omega}{\partial x} = a\cos(ax)C_y E_z ∂2ω∂x2=−a2sin⁡(ax)CyEz=−a2ω\frac{\partial^2 \omega}{\partial x^2} = -a^2\sin(ax)C_y E_z = -a^2\omega
  2. Calculate the first and second partial derivatives of ω\omega with respect to yy.

    Let Sx=sin⁡(ax)S_x = \sin(ax) and Ez=e−a2+b2zE_z = e^{-\sqrt{a^2+b^2}z}. Then ω=Sxcos⁡(by)Ez\omega = S_x \cos(by) E_z.

    ∂ω∂y=Sx(−bsin⁡(by))Ez=−bsin⁡(ax)sin⁡(by)Ez\frac{\partial \omega}{\partial y} = S_x (-b\sin(by)) E_z = -b\sin(ax)\sin(by)E_z ∂2ω∂y2=Sx(−b2cos⁡(by))Ez=−b2sin⁡(ax)cos⁡(by)Ez=−b2ω\frac{\partial^2 \omega}{\partial y^2} = S_x (-b^2\cos(by)) E_z = -b^2\sin(ax)\cos(by)E_z = -b^2\omega
  3. Calculate the first and second partial derivatives of ω\omega with respect to zz.

    Let Sx=sin⁡(ax)S_x = \sin(ax) and Cy=cos⁡(by)C_y = \cos(by). Let k=a2+b2k = \sqrt{a^2+b^2}. Then ω=SxCye−kz\omega = S_x C_y e^{-kz}.

    ∂ω∂z=SxCy(−ke−kz)=−ksin⁡(ax)cos⁡(by)e−kz\frac{\partial \omega}{\partial z} = S_x C_y (-k e^{-kz}) = -k\sin(ax)\cos(by)e^{-kz} ∂2ω∂z2=SxCy(−k)(−ke−kz)=k2sin⁡(ax)cos⁡(by)e−kz=k2ω\frac{\partial^2 \omega}{\partial z^2} = S_x C_y (-k)(-k e^{-kz}) = k^2\sin(ax)\cos(by)e^{-kz} = k^2\omega

    Substitute k=a2+b2k = \sqrt{a^2+b^2}:

    ∂2ω∂z2=(a2+b2)2ω=(a2+b2)ω\frac{\partial^2 \omega}{\partial z^2} = (\sqrt{a^2+b^2})^2\omega = (a^2+b^2)\omega
  4. Sum the second partial derivatives to check Laplace's equation.

    ∂2ω∂x2+∂2ω∂y2+∂2ω∂z2=−a2ω−b2ω+(a2+b2)ω\frac{\partial^2 \omega}{\partial x^2} + \frac{\partial^2 \omega}{\partial y^2} + \frac{\partial^2 \omega}{\partial z^2} = -a^2\omega - b^2\omega + (a^2+b^2)\omega =(−a2−b2+a2+b2)ω=0ω=0= (-a^2 - b^2 + a^2 + b^2)\omega = 0\omega = 0

    Since the sum is 0, the function ω\omega satisfies Laplace's equation.

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