Laplacian and gradient in curvilinear coordinates

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Given x=rcos⁡φx=r\cos \varphi, y=rsin⁡φy=r\sin \varphi, transform the following expression into polar coordinates rr and φ\varphi: w=(∂u∂x)2+(∂u∂y)2w=\left(\dfrac {\partial u}{\partial x}\right)^{2}+\left(\dfrac {\partial u}{\partial y}\right)^{2}.

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Given x=rcos⁡φx=r\cos \varphi, y=rsin⁡φy=r\sin \varphi, transform the following expression into polar coordinates rr and φ\varphi: w=∂2u∂x2+∂2u∂y2w=\dfrac {\partial^{2}u}{\partial x^{2}}+\dfrac {\partial^{2}u}{\partial y^{2}}.

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Take uu and vv as new independent variables, and transform the following equation: ∂2z∂x2+∂2z∂y2+m2z=0\dfrac {\partial^{2}z}{\partial x^{2}}+\dfrac {\partial^{2}z}{\partial y^{2}}+m^{2}z=0, where x=eucos⁡vx=e^{u}\cos v, y=eusin⁡vy=e^{u}\sin v.

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Suppose u=f(r)u=f(r), where r=x2+y2r=\sqrt{x^{2}+y^{2}}, transform the equations

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(a)

Δu≡∂2u∂x2+∂2u∂y2=0\Delta u \equiv \dfrac {\partial^{2}u}{\partial x^{2}}+\dfrac {\partial^{2}u}{\partial y^{2}}=0;

(b)

Δ(Δu)=0\Delta (\Delta u)=0.

Given

x=rsin⁡θcos⁡φ,y=rsin⁡θsin⁡φ,z=rcos⁡θ, x=r\sin \theta \cos \varphi , \quad y=r\sin \theta \sin \varphi , \quad z=r\cos \theta ,

express the quantities Δ1u=(∂u∂x)2+(∂u∂y)2+(∂u∂z)2\Delta_{1}u=\left(\dfrac {\partial u}{\partial x}\right)^{2}+\left(\dfrac {\partial u}{\partial y}\right)^{2}+\left(\dfrac {\partial u}{\partial z}\right)^{2} and Δ2u=∂2u∂x2+∂2u∂y2+∂2u∂z2\Delta_{2}u=\dfrac {\partial^{2}u}{\partial x^{2}}+\dfrac {\partial^{2}u}{\partial y^{2}}+\dfrac {\partial^{2}u}{\partial z^{2}} in terms of spherical coordinates.

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Find the expression for the divergence of a plane vector a→=a→(r,φ)\overrightarrow {a}=\overrightarrow {a}(r,\varphi ) represented in polar coordinates rr and φ\varphi.

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Let

x=f(u,v,w),y=g(u,v,w),z=h(u,v,w), x=f(u,v,w) , \qquad y=g(u,v,w) , \qquad z=h(u,v,w) ,

express div⁡a→(x,y,z)\operatorname {div}\overrightarrow {a}(x,y,z) in orthogonal curvilinear coordinates uu, vv, ww.

As special cases, find the expressions for div⁡a→\operatorname {div}\overrightarrow {a} in cylindrical coordinates and in spherical coordinates.

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Transform to polar coordinates, setting x=rcos⁡φx = r\cos \varphi, y=rsin⁡φy = r\sin \varphi, the expression w=(∂u∂x)2+(∂u∂y)2w = \left(\frac{\partial u}{\partial x}\right)^{2}+\left(\frac{\partial u}{\partial y}\right)^{2}.

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Transform to polar coordinates, setting x=rcos⁡φx = r\cos \varphi, y=rsin⁡φy = r\sin \varphi, the expression w=∂2u∂x2+∂2u∂y2w = \frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}.

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What form does the equation ∂2u∂x2+∂2u∂y2+u=0\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}+u = 0 take, if u=φ(r)u = \varphi (r), where r=x2+y2r = \sqrt{x^{2}+y^{2}}?

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The same question for the equation

∂4u∂x4+2∂4u∂x2∂y2+∂4u∂y4=0. \frac{\partial ^{4} u}{\partial x^{4}}+2\frac{\partial ^{4} u}{\partial x^{2} \partial y^{2}}+\frac{\partial ^{4} u}{\partial y^{4}} = 0.
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What form does the equation ∂2u∂x2+∂2u∂y2+∂2u∂z2+u=0\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}+\frac{\partial^{2} u}{\partial z^{2}}+u = 0 take, if u=φ(r)u = \varphi (r), r=x2+y2+z2r = \sqrt{x^{2}+y^{2}+z^{2}}?

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Transform the expressions

Δ1v=(∂v∂x)2+(∂v∂y)2+(∂v∂z)2 \Delta _{1}v = \left(\frac{\partial v}{\partial x}\right)^{2}+\left(\frac{\partial v}{\partial y}\right)^{2}+\left(\frac{\partial v}{\partial z}\right)^{2}

and

Δ2v=∂2v∂x2+∂2v∂y2+∂2v∂z2 \Delta _{2}v = \frac{\partial ^{2} v}{\partial x^{2}}+\frac{\partial ^{2} v}{\partial y^{2}}+\frac{\partial ^{2} v}{\partial z^{2}}

to spherical coordinates, setting

x=rsin⁡θcos⁡φ,y=rsin⁡θsin⁡φ,z=vcos⁡θ. x = r\sin \theta \cos \varphi , \qquad y = r\sin \theta \sin \varphi , \qquad z = v\cos \theta .
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Express grad⁡u\operatorname {grad} u :

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(1)

in cylindrical coordinates r,φ,zr, \varphi , z;

(2)

in spherical coordinates r,φ,ψr, \varphi , \psi, using the corresponding unit vectors er,eφ,ez\mathbf{e}_{r}, \mathbf{e}_{\varphi }, \mathbf{e}_{z} and er,eφ,eψ\mathbf{e}_{r}, \mathbf{e}_{\varphi }, \mathbf{e}_{\psi }, tangent to the coordinate lines.

Find div⁡\operatorname {div} a of the plane field a in polar coordinates.

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Find div a of a three-dimensional field:

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(1)

in cylindrical coordinates;

(2)

in spherical coordinates.

Find the components of rot⁡a\operatorname {rot} \mathbf{a} of the plane field a in polar coordinates.

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Find the components of rot⁡a\operatorname {rot} \mathbf{a} of a three-dimensional field a:

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(1)

in cylindrical coordinates;

(2)

in spherical coordinates.

Write Δu=div⁡grad⁡u\Delta u = \operatorname {div} \operatorname {grad} u :

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(1)

in cylindrical coordinates;

(2)

in spherical coordinates.

Let an orthogonal system of curvilinear coordinates (ξ;η;ζ)(\xi ; \eta ; \zeta ) be introduced in the region Ω\Omega :

x=x(ξ;η;ζ),y=y(ξ;η;ζ),z=z(ξ;η;ζ) x = x(\xi ; \eta ; \zeta ), \quad y = y(\xi ; \eta ; \zeta ), \quad z = z(\xi ; \eta ; \zeta )

where the right-hand sides are continuously differentiable functions. Let eξ,eη,eζ\mathbf{e}_{\xi }, \mathbf{e}_{\eta }, \mathbf{e}_{\zeta } be the unit vectors of this system (vectors tangent to the coordinate lines and directed toward increasing coordinates, eξ⊥eη,eη⊥eζ,eζ⊥eξ\mathbf{e}_{\xi } \perp \mathbf{e}_{\eta }, \mathbf{e}_{\eta } \perp \mathbf{e}_{\zeta }, \mathbf{e}_{\zeta } \perp \mathbf{e}_{\xi })∗^{*}. Let Hξ,Hη,HζH_{\xi }, H_{\eta }, H_{\zeta } be the Lame coefficients, i.e. Hξ=(∂x∂ξ)2+(∂y∂ξ)2+(∂z∂ξ)2H_{\xi } = \sqrt{\left(\frac{\partial x}{\partial \xi }\right)^{2}+\left(\frac{\partial y}{\partial \xi }\right)^{2}+\left(\frac{\partial z}{\partial \xi }\right)^{2}} etc. Prove that:

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(1)

grad⁡u=1Hξ∂u∂ξeξ+1Hη∂u∂ηeη+1Hζ∂u∂ζeζ\operatorname {grad} u = \frac{1}{H_{\xi }} \frac{\partial u}{\partial \xi } \mathbf{e}_{\xi }+\frac{1}{H_{\eta }} \frac{\partial u}{\partial \eta } \mathbf{e}_{\eta }+\frac{1}{H_{\zeta }} \frac{\partial u}{\partial \zeta } \mathbf{e}_{\zeta };

(2)

div⁡a=1HξHηHζ(∂(HηHζaξ)∂ξ+∂(HζHξaη)∂η+∂(HξHηaζ)∂ζ)\operatorname {div} \mathbf{a} = \dfrac {1}{H_{\xi } H_{\eta } H_{\zeta }}\left(\dfrac {\partial \left(H_{\eta } H_{\zeta } a_{\xi }\right)}{\partial \xi }+\dfrac {\partial \left(H_{\zeta } H_{\xi } a_{\eta }\right)}{\partial \eta }+\dfrac {\partial \left(H_{\xi } H_{\eta } a_{\zeta }\right)}{\partial \zeta }\right);

(3)

rot⁡a=1HξHηHζ∣HξeξHηeηHζeζ∂∂ξ∂∂η∂∂ζHξaξHηaηHζaζ∣\operatorname {rot} \mathbf{a} = \dfrac {1}{H_{\xi } H_{\eta } H_{\zeta }} \begin{vmatrix} H_{\xi } \mathbf{e}_{\xi } & H_{\eta } \mathbf{e}_{\eta } & H_{\zeta } \mathbf{e}_{\zeta } \\ \frac{\partial }{\partial \xi } & \frac{\partial }{\partial \eta } & \frac{\partial }{\partial \zeta } \\ H_{\xi } a_{\xi } & H_{\eta } a_{\eta } & H_{\zeta } a_{\zeta }\end{vmatrix}

Here, for orthogonal curvilinear coordinates (ξ;η;ζ)(\xi ; \eta ; \zeta ) with unit vectors eξ,eη,eζ\mathbf{e}_{\xi }, \mathbf{e}_{\eta }, \mathbf{e}_{\zeta } and Lame coefficients Hξ,Hη,HζH_{\xi }, H_{\eta }, H_{\zeta } (see problem 66), formulas (39)-(41) are

grad⁡u=1Hξ∂u∂ξeξ+1Hη∂u∂ηeη+1Hζ∂u∂ζeζ,(39) \operatorname {grad} u = \frac{1}{H_{\xi }} \frac{\partial u}{\partial \xi } \mathbf{e}_{\xi }+\frac{1}{H_{\eta }} \frac{\partial u}{\partial \eta } \mathbf{e}_{\eta }+\frac{1}{H_{\zeta }} \frac{\partial u}{\partial \zeta } \mathbf{e}_{\zeta }, \quad (39) div⁡a=1HξHηHζ(∂(HηHζaξ)∂ξ+∂(HζHξaη)∂η+∂(HξHηaζ)∂ζ),(40) \operatorname {div} \mathbf{a} = \dfrac {1}{H_{\xi } H_{\eta } H_{\zeta }}\left(\dfrac {\partial \left(H_{\eta } H_{\zeta } a_{\xi }\right)}{\partial \xi }+\dfrac {\partial \left(H_{\zeta } H_{\xi } a_{\eta }\right)}{\partial \eta }+\dfrac {\partial \left(H_{\xi } H_{\eta } a_{\zeta }\right)}{\partial \zeta }\right), \quad (40) rot⁡a=1HξHηHζ∣HξeξHηeηHζeζ∂∂ξ∂∂η∂∂ζHξaξHηaηHζaζ∣.(41) \operatorname {rot} \mathbf{a} = \dfrac {1}{H_{\xi } H_{\eta } H_{\zeta }} \begin{vmatrix} H_{\xi } \mathbf{e}_{\xi } & H_{\eta } \mathbf{e}_{\eta } & H_{\zeta } \mathbf{e}_{\zeta } \\ \frac{\partial }{\partial \xi } & \frac{\partial }{\partial \eta } & \frac{\partial }{\partial \zeta } \\ H_{\xi } a_{\xi } & H_{\eta } a_{\eta } & H_{\zeta } a_{\zeta }\end{vmatrix}. \quad (41)

Using formulas (39)-(41), derive expressions for grad⁡u,div⁡a,rot⁡a\operatorname {grad} u, \operatorname {div} \mathbf{a}, \operatorname {rot} \mathbf{a} :

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(1)

in cylindrical coordinates;

(2)

in spherical coordinates.

References

[Dem97] Demidovich B.P. Сборник задач и упражнений по математическому анализу. 13-е изд., Издательство Московского университета / Издательство "ЧеРо", 1997.
[ГюКу03] Гюнтер Н.М., Кузьмин Р.О. Сборник задач по высшей математике. 13-е изд., Издательство «Лань», 2003.
[ККЧ+03] Кудрявцев Л.Д., Кутасов А.Д., Чехлов В.И., Шабунин М.И. Функции многих переменных. 2-е изд., ФИЗМАТЛИТ, 2003.