Section 6.4

Change of Variables

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Problem 3431

Taking yy as the new independent variable, transform the equation

y′y−3y′′2=x. y'y-3y''^{2}=x .
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Problem 3432

Using the same method, transform the equation

(y′)2y(4)−10y′y′′y′′′+15(y′′)3=0. (y')^{2}y^{(4)}-10y'y''y'''+15(y'')^{3}=0 .
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Problem 3433

Taking xx as the function and t=xyt=xy as the independent variable, transform the equation

y′′+2xy′+y=0. y''+\dfrac {2}{x}y'+y=0 .
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Problem 3434

Introduce a new variable and transform the following ordinary differential equation: x2y′′+xy′+y=0x^{2}y''+xy'+y=0, if x=etx=e^{t}.

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Problem 3435

Introduce a new variable and transform the following ordinary differential equation: y′′′=6yx3y'''=\dfrac {6y}{x^{3}}, if t=ln⁡∣x∣t=\ln \left|x\right|.

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Problem 3436

Introduce a new variable and transform the following ordinary differential equation: (1−x2)y′′−xy′+n2y=0(1-x^{2})y''-xy'+n^{2}y=0, if x=cos⁡tx=\cos t.

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Problem 3437

Introduce a new variable and transform the following ordinary differential equation: y′′+y′tanh⁡x+m2cosh⁡2xy=0y''+y'\tanh x+\dfrac {m^{2}}{\cosh^{2}x}y=0, if x=ln⁡tan⁡t2x=\ln \tan \dfrac {t}{2}.

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Problem 3438

Introduce a new variable and transform the following ordinary differential equation: y′′+p(x)y′+q(x)y=0y''+p(x)y'+q(x)y=0, let y=ue−12∫x0xp(ξ)dξy=ue^{-\frac{1}{2}\int_{x_{0}}^{x} p(\xi )d\xi }.

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Problem 3439

Introduce a new variable and transform the following ordinary differential equation: x4y′′+xyy′−2y2=0x^{4}y''+xyy'-2y^{2}=0. Let

x=et,y=ue2t, x=e^{t} , \quad y=ue^{2t} ,

where u=u(t)u=u(t).

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Problem 3440

Introduce a new variable and transform the following ordinary differential equation: (1+x2)2y′′=y(1+x^{2})^{2}y''=y, if

x=tan⁡t,y=ucos⁡t, x=\tan t , \quad y=\dfrac {u}{\cos t} ,

where u=u(t)u=u(t).

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Problem 3441

Introduce a new variable and transform the following ordinary differential equation: (1−x2)2y′′=−y(1-x^{2})^{2}y''=-y, if

x=tanh⁡t,y=ucosh⁡t, x=\tanh t , \quad y=\dfrac {u}{\cosh t} ,

where u=u(t)u=u(t).

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Problem 3442

Introduce a new variable and transform the following ordinary differential equation: y′′+(x+y)(1+y′)3=0y''+(x+y)(1+y')^{3}=0, if x=u+tx=u+t, y=u−ty=u-t, where u=u(t)u=u(t).

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Problem 3443

Introduce a new variable and transform the following ordinary differential equation: y′′′−x3y′′+xy′−y=0y'''-x^{3}y''+xy'-y=0, if x=1tx=\dfrac {1}{t} and y=uty=\dfrac {u}{t}, where u=u(t)u=u(t).

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Problem 3444

Suppose

u=yx−b,t=ln⁡∣x−ax−b∣, u=\dfrac {y}{x-b} , \quad t=\ln \left|\dfrac {x-a}{x-b}\right| ,

and take uu as a function of the variable tt, to transform the Stokes equation

y′′=−Ay(x−a)2(x−b)2. y''=-\dfrac {Ay}{(x-a)^{2}(x-b)^{2}} .
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Problem 3445

Prove: if the equation

d2ydx2+p(x)dydx+q(x)y=0, \dfrac {d^{2}y}{dx^{2}}+p(x)\dfrac {dy}{dx}+q(x)y=0 ,

is transformed by the substitution x=φ(ξ)x=\varphi (\xi ) into the equation

d2ydξ2+P(ξ)dydξ+Q(ξ)y=0, \dfrac {d^{2}y}{d\xi ^{2}}+P(\xi )\dfrac {dy}{d\xi }+Q(\xi )y=0 ,

then

[2P(ξ)Q(ξ)+Q′(ξ)][Q(ξ)]−32=[2p(x)q(x)+q′(x)][q(x)]−32. \begin{align} & \left[2P(\xi )Q(\xi )+Q'(\xi )\right]\left[Q(\xi )\right]^{-\frac{3}{2}} \\ & =\left[2p(x)q(x)+q'(x)\right]\left[q(x)\right]^{-\frac{3}{2}} . \end{align}
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Problem 3446

In the equation

Φ(y,y′,y′′)=0 \Phi (y, y', y'')=0

(where Φ\Phi is a homogeneous function of the variables yy, y′y', y′′y''), let y=e∫x0xu dxy=e^{\int_{x_{0}}^{x} u\, dx}.

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Problem 3447

In the equation

F(x2y′′,xy′,y)=0 F(x^{2}y'', xy', y)=0

(where FF is a homogeneous function of its variables), let u=x⋅y’yu=x \cdot \dfrac {y’}{y}.

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Problem 3448

Prove: under the projective transformation

x=a1ξ+b1η+c1aξ+bη+c,y=a2ξ+b2η+c2aξ+bη+c, x=\dfrac {a_{1}\xi +b_{1}\eta +c_{1}}{a\xi +b\eta +c} , \quad y=\dfrac {a_{2}\xi +b_{2}\eta +c_{2}}{a\xi +b\eta +c} ,

the equation

y′′(1+y′2)−3y′y′′2=0 y''(1+y'^{2})-3y'y''^{2}=0

does not change its form.

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Problem 3449

Prove:

S[x(t)]=x”’(t)x’(t)−32[x”(t)x’(t)]2 S\left[x(t)\right]=\dfrac {x”’(t)}{x’(t)}-\dfrac {3}{2}\left[\dfrac {x”(t)}{x’(t)}\right]^{2}

is invariant under the linear fractional transformation

y=ax(t)+bcx(t)+d(ad−bc≠0). y=\dfrac {ax(t)+b}{cx(t)+d} \quad (ad-bc \neq 0) .
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Problem 3450

Transform the following equation into an equation expressed in polar coordinates rr and φ\varphi, i.e. let x=rcos⁡φx=r\cos \varphi, y=rsin⁡φy=r\sin \varphi:

dydx=x+yx−y. \dfrac {dy}{dx}=\dfrac {x+y}{x-y} .
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Problem 3451

Transform the following equation into an equation expressed in polar coordinates rr and φ\varphi:

(xy′−y)2=2xy(1+y′2). (xy'-y)^{2}=2xy(1+y'^{2}) .
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Problem 3452

Transform the following equation into an equation expressed in polar coordinates rr and φ\varphi:

(x2+y2)2y′′=(x+yy′)3. (x^{2}+y^{2})^{2}y''=(x+yy')^{3} .
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Problem 3453

Transform the expression

x+yy’xy’−y \dfrac {x+yy’}{xy’-y}

into an expression in polar coordinates.

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Problem 3454

Express the curvature of a plane curve

K=∣yxx”∣(1+yx’2)32 K=\dfrac {\left|y_{xx}”\right|}{(1+y_{x}’^{2})^{\frac{3}{2}}}

in terms of polar coordinates rr and φ\varphi.

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Problem 3455

Transform the system of equations

dxdt=y+kx(x2+y2), \dfrac {dx}{dt}=y+kx(x^{2}+y^{2}) , dydt=−x+ky(x2+y2) \dfrac {dy}{dt}=-x+ky(x^{2}+y^{2})

into a system of equations in polar coordinates.

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Problem 3456

Introduce the new functions r=x2+y2r=\sqrt{x^{2}+y^{2}}, φ=arctan⁡yx\varphi =\arctan \dfrac {y}{x}, and transform the expression

W=xd2ydt2−yd2xdt2. W=x\dfrac {d^{2}y}{dt^{2}}-y\dfrac {d^{2}x}{dt^{2}} .
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Problem 3457

In the Legendre transformation, each point (x,y)(x,y) of the curve y=y(x)y=y(x) corresponds to a point (X,Y)(X,Y), where

X=y′,Y=xy′−y. X=y' , \quad Y=xy'-y .

Find Y′Y', Y′′Y'' and Y′′′Y'''.

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Problem 3458

Introduce new variables ξ\xi and η\eta, and solve the following equation: ∂z∂x=∂z∂y\dfrac {\partial z}{\partial x}=\dfrac {\partial z}{\partial y}, let ξ=x+y\xi =x+y, η=x−y\eta =x-y.

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Problem 3459

Introduce new variables ξ\xi and η\eta, and solve the following equation: y∂z∂x−x∂z∂y=0y\dfrac {\partial z}{\partial x}-x\dfrac {\partial z}{\partial y}=0, let ξ=x\xi =x, η=x2+y2\eta =x^{2}+y^{2}.

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Problem 3460

Introduce new variables ξ\xi and η\eta, and solve the following equation: a∂z∂x+b∂z∂y=1a\dfrac {\partial z}{\partial x}+b\dfrac {\partial z}{\partial y}=1 (a≠0)(a \neq 0), let ξ=x\xi =x, η=y−bz\eta =y-bz.

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Problem 3461

Introduce new variables ξ\xi and η\eta, and solve the following equation: x∂z∂x+y∂z∂y=zx\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}=z, let ξ=x\xi =x and η=yx\eta =\dfrac {y}{x}.

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Problem 3462

Take uu and vv as new independent variables, and transform the following equation: x∂z∂x+1+y2∂z∂y=xyx\dfrac {\partial z}{\partial x}+\sqrt{1+y^{2}}\dfrac {\partial z}{\partial y}=xy, if u=ln⁡xu=\ln x, v=ln⁡(y+1+y2)v=\ln (y+\sqrt{1+y^{2}}).

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Problem 3463

Take uu and vv as new independent variables, and transform the following equation: (x+y)∂z∂x−(x−y)∂z∂y=0(x+y)\dfrac {\partial z}{\partial x}-(x-y)\dfrac {\partial z}{\partial y}=0, if u=ln⁡x2+y2u=\ln \sqrt{x^{2}+y^{2}}, v=arctan⁡yxv=\arctan \dfrac {y}{x}.

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Problem 3464

Take uu and vv as the new independent variables, and transform the following equation: x∂z∂x+y∂z∂y=z+x2+y2+z2x\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}=z+\sqrt{x^{2}+y^{2}+z^{2}}, if u=yxu=\dfrac {y}{x}, v=z+x2+y2+z2v=z+\sqrt{x^{2}+y^{2}+z^{2}}.

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Problem 3465

Take uu and vv as the new independent variables, and transform the following equation: x∂z∂x+y∂z∂y=xzx\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}=\dfrac {x}{z}, if u=2x−z2u=2x-z^{2}, v=yzv=\dfrac {y}{z}.

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Problem 3466

Take uu and vv as the new independent variables, and transform the following equation: (x+z)∂z∂x+(y+z)∂z∂y=x+y+z(x+z)\dfrac {\partial z}{\partial x}+(y+z)\dfrac {\partial z}{\partial y}=x+y+z, if u=x+zu=x+z, v=y+zv=y+z.

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Problem 3467

Take

ξ=y+ze−x,η=x+ze−y \xi =y+ze^{-x} , \quad \eta =x+ze^{-y}

as the new independent variables, and transform the expression

(z+ex)∂z∂x+(z+ey)∂z∂y−(z2−ex+y). (z+e^{x})\dfrac {\partial z}{\partial x}+(z+e^{y})\dfrac {\partial z}{\partial y}-(z^{2}-e^{x+y}) .
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Problem 3468

Suppose

x=uv,y=12(u2−v2) x=uv , \quad y=\dfrac {1}{2}(u^{2}-v^{2})

transform the expression

(∂z∂x)2+(∂z∂y)2. \left(\dfrac {\partial z}{\partial x}\right)^{2}+\left(\dfrac {\partial z}{\partial y}\right)^{2} .
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Problem 3469

In the equation

∂u∂x+∂u∂y+∂u∂z=0 \dfrac {\partial u}{\partial x}+\dfrac {\partial u}{\partial y}+\dfrac {\partial u}{\partial z}=0

set ξ=x\xi =x, η=y−x\eta =y-x, ζ=z−x\zeta =z-x.

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Problem 3470

Take xx as the function, and yy and zz as the independent variables, and transform the equation

(x−z)∂z∂x+y∂z∂y=0. (x-z)\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}=0 .
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Problem 3471

Take xx as the function, and u=y−zu=y-z, v=y+zv=y+z as the independent variables, and transform the equation

(y−z)∂z∂x+(y+z)∂z∂y=0. (y-z)\dfrac {\partial z}{\partial x}+(y+z)\dfrac {\partial z}{\partial y}=0 .
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Problem 3472

Take xx as the function, and u=xzu=xz, v=yzv=yz as the independent variables, and transform the expression

A=(∂z∂x)2+(∂z∂y)2. A=\left(\dfrac {\partial z}{\partial x}\right)^{2}+\left(\dfrac {\partial z}{\partial y}\right)^{2} .
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Problem 3473

In the equation

(y+z+u)∂u∂x+(x+z+u)∂u∂y+(x+y+u)∂u∂z=x+y+z \begin{align} (y+z+u)\dfrac {\partial u}{\partial x} & +(x+z+u)\dfrac {\partial u}{\partial y} \\ & +(x+y+u)\dfrac {\partial u}{\partial z}=x+y+z \end{align}

set eξ=x−ue^{\xi }=x-u, eη=y−ue^{\eta }=y-u, eζ=z−ue^{\zeta }=z-u.

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Problem 3474

In the following equation, substitute the new variables uu, vv, ww, where w=w(u,v)w=w(u,v): y∂z∂x−x∂z∂y=(y−x)zy\dfrac {\partial z}{\partial x}-x\dfrac {\partial z}{\partial y}=(y-x)z, set u=x2+y2u=x^{2}+y^{2}, v=1x+1yv=\dfrac {1}{x}+\dfrac {1}{y}, w=ln⁡z−(x+y)w=\ln z-(x+y).

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Problem 3475

In the following equation, substitute the new variables uu, vv, ww, where w=w(u,v)w=w(u,v): x2∂z∂x+y2∂z∂y=z2x^{2}\dfrac {\partial z}{\partial x}+y^{2}\dfrac {\partial z}{\partial y}=z^{2}, set u=xu=x, v=1y−1xv=\dfrac {1}{y}-\dfrac {1}{x}, w=1z−1xw=\dfrac {1}{z}-\dfrac {1}{x}.

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Problem 3476

In the following equation, substitute the new variables uu, vv, ww, where w=w(u,v)w=w(u,v): (xy+z)∂z∂x+(1−y2)∂z∂y=x+yz(xy+z)\dfrac {\partial z}{\partial x}+(1-y^{2})\dfrac {\partial z}{\partial y}=x+yz, let u=yz−xu=yz-x, v=xz−yv=xz-y, w=xy−zw=xy-z.

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Problem 3477

In the following equation, substitute the new variables uu, vv, ww, where w=w(u,v)w=w(u,v): (x∂z∂x)2+(y∂z∂y)2=z2∂z∂x∂z∂y\left(x\dfrac {\partial z}{\partial x}\right)^{2}+\left(y\dfrac {\partial z}{\partial y}\right)^{2}=z^{2}\dfrac {\partial z}{\partial x}\dfrac {\partial z}{\partial y}, set x=uewx=ue^{w}, y=vewy=ve^{w}, z=wewz=we^{w}.

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Problem 3478

Suppose u=ln⁡x2+y2u=\ln \sqrt{x^{2}+y^{2}}, v=arctan⁡zv=\arctan z, w=x+y+zw=x+y+z, where w=w(u,v)w=w(u,v), transform the expression

(x−y):(∂z∂x−∂z∂y). (x-y):\left(\dfrac {\partial z}{\partial x}-\dfrac {\partial z}{\partial y}\right) .
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Problem 3479

Suppose u=xezu=xe^{z}, v=yezv=ye^{z}, w=zezw=ze^{z}, where w=w(u,v)w=w(u,v), transform the expression

A=∂z∂x⋅∂z∂y. A=\dfrac {\partial z}{\partial x} \cdot \dfrac {\partial z}{\partial y} .
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Problem 3480

In the equation

x∂u∂x+y∂u∂y+z∂u∂z=u+xyz x\dfrac {\partial u}{\partial x}+y\dfrac {\partial u}{\partial y}+z\dfrac {\partial u}{\partial z}=u+\dfrac {xy}{z}

set ξ=xz\xi =\dfrac {x}{z}, η=yz\eta =\dfrac {y}{z}, ζ=z\zeta =z, w=uzw=\dfrac {u}{z}, where w=w(ξ,η,ζ)w=w(\xi ,\eta ,\zeta ).

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Problem 3481

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=x∂u∂y−y∂u∂xw=x\dfrac {\partial u}{\partial y}-y\dfrac {\partial u}{\partial x}.

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Problem 3482

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=x∂u∂x+y∂u∂yw=x\dfrac {\partial u}{\partial x}+y\dfrac {\partial u}{\partial y}.

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Problem 3483

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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Problem 3484

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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Problem 3485

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=x2∂2u∂x2+2xy∂2u∂x∂y+y2∂2u∂y2w=x^{2}\dfrac {\partial^{2}u}{\partial x^{2}}+2xy\dfrac {\partial^{2}u}{\partial x \partial y}+y^{2}\dfrac {\partial^{2}u}{\partial y^{2}}.

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Problem 3486

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=y2∂2z∂x2−2xy∂2z∂x∂y+x2∂2z∂y2−(x∂z∂x+y∂z∂y). w=y^{2}\dfrac {\partial ^{2}z}{\partial x^{2}}-2xy\dfrac {\partial ^{2}z}{\partial x \partial y}+x^{2}\dfrac {\partial ^{2}z}{\partial y^{2}}-\left(x\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}\right) .
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Problem 3487

In the expression

I=∂u∂x∂v∂y−∂u∂y∂v∂x I=\dfrac {\partial u}{\partial x}\dfrac {\partial v}{\partial y}-\dfrac {\partial u}{\partial y}\dfrac {\partial v}{\partial x}

let x=rcos⁡φx=r\cos \varphi, y=rsin⁡φy=r\sin \varphi.

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Problem 3488

Introduce the new independent variables

ξ=x−at,η=x+at \xi =x-at , \quad \eta =x+at

and solve the equation

∂2u∂t2=a2⋅∂2u∂x2. \dfrac {\partial ^{2}u}{\partial t^{2}}=a^{2} \cdot \dfrac {\partial ^{2}u}{\partial x^{2}} .
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Problem 3489

Take uu and vv as new independent variables, and transform the following equation: 2∂2z∂x2+∂2z∂x∂y−∂2z∂y2+∂z∂x+∂z∂y=02\dfrac {\partial^{2}z}{\partial x^{2}}+\dfrac {\partial^{2}z}{\partial x \partial y}-\dfrac {\partial^{2}z}{\partial y^{2}}+\dfrac {\partial z}{\partial x}+\dfrac {\partial z}{\partial y}=0, where u=x+2y+2u=x+2y+2 and v=x−y−1v=x-y-1.

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Problem 3490

Take uu and vv as new independent variables, and transform the following equation: (1+x2)∂2z∂x2+(1+y2)∂2z∂y2+x∂z∂x+y∂z∂y=0(1+x^{2})\dfrac {\partial^{2}z}{\partial x^{2}}+(1+y^{2})\dfrac {\partial^{2}z}{\partial y^{2}}+x\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}=0, where u=ln⁡(x+1+x2)u=\ln (x+\sqrt{1+x^{2}}) and v=ln⁡(y+1+y2)v=\ln (y+\sqrt{1+y^{2}}).

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Problem 3491

Take uu and vv as new independent variables, and transform the following equation: ax2∂2z∂x2+2bxy∂2z∂x∂y+cy2∂2z∂y2=0ax^{2}\dfrac {\partial^{2}z}{\partial x^{2}}+2bxy\dfrac {\partial^{2}z}{\partial x \partial y}+cy^{2}\dfrac {\partial^{2}z}{\partial y^{2}}=0 (aa, bb, cc are constants), where u=ln⁡xu=\ln x, v=ln⁡yv=\ln y.

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Problem 3492

Take uu and vv as new independent variables, and transform the following equation: ∂2z∂x2+∂2z∂y2=0\dfrac {\partial^{2}z}{\partial x^{2}}+\dfrac {\partial^{2}z}{\partial y^{2}}=0, where u=xx2+y2u=\dfrac {x}{x^{2}+y^{2}}, v=−yx2+y2v=-\dfrac {y}{x^{2}+y^{2}}.

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Problem 3493

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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Problem 3494

Take uu and vv as new independent variables, and transform the following equation: ∂2z∂x2−y∂2z∂y2=12∂z∂y\dfrac {\partial^{2}z}{\partial x^{2}}-y\dfrac {\partial^{2}z}{\partial y^{2}}=\dfrac {1}{2}\dfrac {\partial z}{\partial y} (y>0)(y>0), where u=x−2yu=x-2\sqrt{y} and v=x+2yv=x+2\sqrt{y}.

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Problem 3495

Take uu and vv as new independent variables, and transform the following equation: x2∂2z∂x2−y2∂2z∂y2=0x^{2}\dfrac {\partial^{2}z}{\partial x^{2}}-y^{2}\dfrac {\partial^{2}z}{\partial y^{2}}=0, where u=xyu=xy, v=xyv=\dfrac {x}{y}.

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Problem 3496

Take uu and vv as new independent variables, and transform the following equation: x2∂2z∂x2−(x2+y2)∂2z∂x∂y+y2∂2z∂y2=0x^{2}\dfrac {\partial^{2}z}{\partial x^{2}}-(x^{2}+y^{2})\dfrac {\partial^{2}z}{\partial x \partial y}+y^{2}\dfrac {\partial^{2}z}{\partial y^{2}}=0, where u=x+yu=x+y, v=1x+1yv=\dfrac {1}{x}+\dfrac {1}{y}.

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Problem 3497

Take uu and vv as new independent variables, and transform the following equation:

xy∂2z∂x2−(x2+y2)∂2z∂x∂y+xy∂2z∂y2+y∂z∂x+x∂z∂y=0, xy\dfrac {\partial ^{2}z}{\partial x^{2}}-(x^{2}+y^{2})\dfrac {\partial ^{2}z}{\partial x \partial y}+xy\dfrac {\partial ^{2}z}{\partial y^{2}}+y\dfrac {\partial z}{\partial x}+x\dfrac {\partial z}{\partial y}=0 ,

where u=12(x2+y2)u=\dfrac {1}{2}(x^{2}+y^{2}) and v=xyv=xy.

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Problem 3498

Take uu and vv as new independent variables, and transform the following equation: x2∂2z∂x2−2xsin⁡y∂2z∂x∂y+sin⁡2y∂2z∂y2=0x^{2}\dfrac {\partial^{2}z}{\partial x^{2}}-2x\sin y\dfrac {\partial^{2}z}{\partial x \partial y}+\sin^{2}y\dfrac {\partial^{2}z}{\partial y^{2}}=0, where u=xtan⁡y2u=x\tan \dfrac {y}{2}, v=xv=x.

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Problem 3499

Take uu and vv as the new independent variables and transform the following equation: x∂2z∂x2−y∂2z∂y2=0x\dfrac {\partial^{2}z}{\partial x^{2}}-y\dfrac {\partial^{2}z}{\partial y^{2}}=0 (x>0,y>0)(x>0, y>0), where x=(u+v)2x=(u+v)^{2} and y=(u−v)2y=(u-v)^{2}.

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Problem 3500

Take uu and vv as the new independent variables and transform the following equation: ∂2z∂x∂y=(1+∂z∂y)3\dfrac {\partial^{2}z}{\partial x \partial y}=\left(1+\dfrac {\partial z}{\partial y}\right)^{3}, where u=xu=x, v=y+zv=y+z.

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Problem 3501

Using the linear transformation

ξ=x+λ1y,η=x+λ2y \xi =x+\lambda _{1}y , \quad \eta =x+\lambda _{2}y

transform the equation

A∂2u∂x2+2B∂2u∂x∂y+C∂2u∂y2=0,(1) A\dfrac {\partial ^{2}u}{\partial x^{2}}+2B\dfrac {\partial ^{2}u}{\partial x \partial y}+C\dfrac {\partial ^{2}u}{\partial y^{2}}=0 , \tag {1}

(where AA, BB and CC are constants and C≠0C \neq 0, AC−B2<0AC-B^{2}<0) into the form

∂2u∂ξ∂η=0. \dfrac {\partial ^{2}u}{\partial \xi \partial \eta }=0 .

Find the general form of the function satisfying equation (1).

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Problem 3502

Prove that Laplace's equation

Δz=∂2z∂x2+∂2z∂y2=0 \Delta z=\dfrac {\partial ^{2}z}{\partial x^{2}}+\dfrac {\partial ^{2}z}{\partial y^{2}}=0

keeps its form unchanged under the nondegenerate change of variables

x=φ(u,v),y=ψ(u,v) x=\varphi (u,v) , \quad y=\psi (u,v)

satisfying the conditions ∂φ∂u=∂ψ∂v\dfrac {\partial \varphi }{\partial u}=\dfrac {\partial \psi }{\partial v}, ∂φ∂v=−∂ψ∂u\dfrac {\partial \varphi }{\partial v}=-\dfrac {\partial \psi }{\partial u}.

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Problem 3503

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.

Problem 3504

If we set

w=f(u), w=f(u) ,

where

u=(x−x0)(y−y0), u=(x-x_{0})(y-y_{0}) ,

into what form does the equation

∂2w∂x∂y+cw=0 \dfrac {\partial ^{2}w}{\partial x \partial y}+cw=0

transform?

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Problem 3505

Suppose

x+y=X,y=XY, x+y=X , \quad y=XY ,

transform the expression A=x∂2u∂x2+y∂2u∂x∂y+∂u∂xA=x\dfrac {\partial^{2}u}{\partial x^{2}}+y\dfrac {\partial^{2}u}{\partial x \partial y}+\dfrac {\partial u}{\partial x}.

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Problem 3506

Prove that the equation

∂2z∂x2+2xy2∂z∂x+2(y−y3)∂z∂y+x2y2z2=0 \dfrac {\partial ^{2}z}{\partial x^{2}}+2xy^{2}\dfrac {\partial z}{\partial x}+2(y-y^{3})\dfrac {\partial z}{\partial y}+x^{2}y^{2}z^{2}=0

keeps its form unchanged under the transformation x=uvx=uv and y=1vy=\dfrac {1}{v}.

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Problem 3507

Prove that the equation

∂2z∂x2+2∂2z∂x∂y+∂2z∂y2=0 \dfrac {\partial ^{2}z}{\partial x^{2}}+2\dfrac {\partial ^{2}z}{\partial x \partial y}+\dfrac {\partial ^{2}z}{\partial y^{2}}=0

keeps its form unchanged under the transformation u=x+zu=x+z and v=y+zv=y+z.

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Problem 3508

Suppose

x=ηζ,y=ξζ,z=ξη, x=\eta \zeta , \quad y=\xi \zeta , \quad z=\xi \eta ,

transform the equation xy∂2u∂x∂y+yz∂2u∂y∂z+xz∂2u∂x∂z=0xy\dfrac {\partial^{2}u}{\partial x \partial y}+yz\dfrac {\partial^{2}u}{\partial y \partial z}+xz\dfrac {\partial^{2}u}{\partial x \partial z}=0.

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Problem 3509

Suppose

y1=x2+x3−x1,y2=x1+x3−x2, y_{1}=x_{2}+x_{3}-x_{1} , \quad y_{2}=x_{1}+x_{3}-x_{2} , y3=x1+x2−x3, y_{3}=x_{1}+x_{2}-x_{3} ,

transform the equation

∂2z∂x12+∂2z∂x22+∂2z∂x32+∂2z∂x1∂x2+∂2z∂x1∂x3+∂2z∂x2∂x3=0. \begin{align} & \dfrac {\partial ^{2}z}{\partial x_{1}^{2}}+\dfrac {\partial ^{2}z}{\partial x_{2}^{2}}+\dfrac {\partial ^{2}z}{\partial x_{3}^{2}}+\dfrac {\partial ^{2}z}{\partial x_{1} \partial x_{2}} \\ & \quad +\dfrac {\partial ^{2}z}{\partial x_{1} \partial x_{3}}+\dfrac {\partial ^{2}z}{\partial x_{2} \partial x_{3}}=0 . \end{align}
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Problem 3510

Given

ξ=yx,η=zx,ζ=y−z, \xi =\dfrac {y}{x} , \quad \eta =\dfrac {z}{x} , \quad \zeta =y-z ,

transform the equation

x2∂2u∂x2+y2∂2u∂y2+z2∂2u∂z2+2xy∂2u∂x∂y+2xz∂2u∂x∂z+2yz∂2u∂y∂z=0. \begin{align} & x^{2}\dfrac {\partial ^{2}u}{\partial x^{2}}+y^{2}\dfrac {\partial ^{2}u}{\partial y^{2}}+z^{2}\dfrac {\partial ^{2}u}{\partial z^{2}}+2xy\dfrac {\partial ^{2}u}{\partial x \partial y} \\ & \quad +2xz\dfrac {\partial ^{2}u}{\partial x \partial z}+2yz\dfrac {\partial ^{2}u}{\partial y \partial z}=0 . \end{align}
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Problem 3511

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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Problem 3512

In the equation

z(∂2z∂x2+∂2z∂y2)=(∂z∂x)2+(∂z∂y)2 z\left(\dfrac {\partial ^{2}z}{\partial x^{2}}+\dfrac {\partial ^{2}z}{\partial y^{2}}\right)=\left(\dfrac {\partial z}{\partial x}\right)^{2}+\left(\dfrac {\partial z}{\partial y}\right)^{2}

introduce a new function ww, given by w=z2w=z^{2}.

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Problem 3513

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, transform the following equation: y∂2z∂y2+2∂z∂y=2xy\dfrac {\partial^{2}z}{\partial y^{2}}+2\dfrac {\partial z}{\partial y}=\dfrac {2}{x}, given u=xyu=\dfrac {x}{y}, v=xv=x, w=xz−yw=xz-y.

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Problem 3514

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, transform the following equation: ∂2z∂x2−2∂2z∂x∂y+∂2z∂y2=0\dfrac {\partial^{2}z}{\partial x^{2}}-2\dfrac {\partial^{2}z}{\partial x \partial y}+\dfrac {\partial^{2}z}{\partial y^{2}}=0, given u=x+yu=x+y, v=yxv=\dfrac {y}{x}, w=zxw=\dfrac {z}{x}.

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Problem 3515

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, transform the following equation: ∂2z∂x2+2∂2z∂x∂y+∂2z∂y2=0\dfrac {\partial^{2}z}{\partial x^{2}}+2\dfrac {\partial^{2}z}{\partial x \partial y}+\dfrac {\partial^{2}z}{\partial y^{2}}=0, given u=x+yu=x+y, v=x−yv=x-y, w=xy−zw=xy-z.

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Problem 3516

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, transform the following equation: ∂2z∂x2+∂2z∂x∂y+∂z∂x=z\dfrac {\partial^{2}z}{\partial x^{2}}+\dfrac {\partial^{2}z}{\partial x \partial y}+\dfrac {\partial z}{\partial x}=z, given u=x+y2u=\dfrac {x+y}{2}, v=x−y2v=\dfrac {x-y}{2}, w=zexw=ze^{x}.

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Problem 3517

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, transform the following equation: ∂2z∂x2−2∂2z∂x∂y+(1+yx)∂2z∂y2=0\dfrac {\partial^{2}z}{\partial x^{2}}-2\dfrac {\partial^{2}z}{\partial x \partial y}+\left(1+\dfrac {y}{x}\right)\dfrac {\partial^{2}z}{\partial y^{2}}=0, given u=xu=x, v=x+yv=x+y, w=x+y+zw=x+y+z.

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Problem 3518

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, transform the following equation: (1−x2)∂2z∂x2+(1−y2)∂2z∂y2=x∂z∂x+y∂z∂y(1-x^{2})\dfrac {\partial^{2}z}{\partial x^{2}}+(1-y^{2})\dfrac {\partial^{2}z}{\partial y^{2}}=x\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}, given x=sin⁡ux=\sin u, y=sin⁡vy=\sin v, z=ewz=e^{w}.

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Problem 3519

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, and transform the following equation: (1−x2)∂2z∂x2−∂2z∂y2−2x∂z∂x−14z=0(1-x^{2})\dfrac {\partial^{2}z}{\partial x^{2}}-\dfrac {\partial^{2}z}{\partial y^{2}}-2x\dfrac {\partial z}{\partial x}-\dfrac {1}{4}z=0 (∣x∣<1)(\left|x\right|<1), where u=12(y+arccos⁡x)u=\dfrac {1}{2}(y+\arccos x), v=12(y−arccos⁡x)v=\dfrac {1}{2}(y-\arccos x), w=z1−x24w=z\sqrt[4]{1-x^{2}}.

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Problem 3520

Take uu and vv as the new independent variables and w=w(u,v,z)w=w(u,v,z) as the new function, and transform the following equation: ∂2z∂x2+∂2z∂y2=2x∂z∂x−y∂z∂yx2−y2−3(x2+y2)z(x2−y2)2\dfrac {\partial^{2}z}{\partial x^{2}}+\dfrac {\partial^{2}z}{\partial y^{2}}=2\dfrac {x\dfrac {\partial z}{\partial x}-y\dfrac {\partial z}{\partial y}}{x^{2}-y^{2}}-\dfrac {3(x^{2}+y^{2})z}{(x^{2}-y^{2})^{2}} (∣x∣>∣y∣)(\left|x\right|>\left|y\right|), where u=x+yu=x+y, v=x−yv=x-y, w=zx2−y2w=\dfrac {z}{\sqrt{x^{2}-y^{2}}}.

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Problem 3521

Prove that any equation

∂2z∂x∂y+a∂z∂x+b∂z∂y+cz=0 \dfrac {\partial ^{2}z}{\partial x \partial y}+a\dfrac {\partial z}{\partial x}+b\dfrac {\partial z}{\partial y}+cz=0

(with aa, bb, cc constants) can be reduced, by the substitution

z=ueαx+βy z=ue^{\alpha x+\beta y}

(where α\alpha and β\beta are constants and u=u(x,y)u=u(x,y)), to the form

∂2u∂x∂y+c1u=0(c1=a constant). \dfrac {\partial ^{2}u}{\partial x \partial y}+c_{1}u=0 \quad (c_{1}=\text{a constant}) .
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Problem 3522

Prove that the equation

∂2u∂x2=∂u∂y \dfrac {\partial ^{2}u}{\partial x^{2}}=\dfrac {\partial u}{\partial y}

keeps its form unchanged under the change of variables

x′=xy,y′=−1y,u=u’ye−x24y x'=\dfrac {x}{y} , \quad y'=-\dfrac {1}{y} , \quad u=\dfrac {u’}{\sqrt{y}}e^{-\frac{x^{2}}{4y}}

(where u′u' is a function of the variables x′x' and y′y').

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Problem 3523

In the equation

q(1+q)∂2z∂x2−(1+p+q+2pq)∂2z∂x∂y+p(1+p)∂2z∂y2=0 \begin{align} & q(1+q)\dfrac {\partial ^{2}z}{\partial x^{2}}-(1+p+q+2pq)\dfrac {\partial ^{2}z}{\partial x \partial y} \\ & \quad +p(1+p)\dfrac {\partial ^{2}z}{\partial y^{2}}=0 \end{align}

(where p=∂z∂xp=\dfrac {\partial z}{\partial x}, q=∂z∂yq=\dfrac {\partial z}{\partial y}), let u=x+zu=x+z, v=y+zv=y+z, w=x+y+zw=x+y+z, and suppose w=w(u,v)w=w(u,v).

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Problem 3524

In the equation

x2∂2u∂x2+y2∂2u∂y2+z2∂2u∂z2=(x∂u∂x)2+(y∂u∂y)2+(z∂u∂z)2 \begin{align} & x^{2}\dfrac {\partial ^{2}u}{\partial x^{2}}+y^{2}\dfrac {\partial ^{2}u}{\partial y^{2}}+z^{2}\dfrac {\partial ^{2}u}{\partial z^{2}}=\left(x\dfrac {\partial u}{\partial x}\right)^{2} \\ & \quad +\left(y\dfrac {\partial u}{\partial y}\right)^{2}+\left(z\dfrac {\partial u}{\partial z}\right)^{2} \end{align}

let x=eξx=e^{\xi }, y=eηy=e^{\eta }, z=eζz=e^{\zeta }, u=ewu=e^{w}, where w=w(ξ,η,ζ)w=w(\xi ,\eta ,\zeta ).

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Problem 3525

Prove that the form of the equation

∂2z∂x2∂2z∂y2−(∂2z∂x∂y)2=0 \dfrac {\partial ^{2}z}{\partial x^{2}}\dfrac {\partial ^{2}z}{\partial y^{2}}-\left(\dfrac {\partial ^{2}z}{\partial x \partial y}\right)^{2}=0

does not depend on which roles the variables xx, yy, and zz respectively play.

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Problem 3526

Take xx as a function of the variables yy and zz, and solve the equation

(∂z∂y)2∂2z∂x2−2∂z∂x∂z∂y∂2z∂x∂y+(∂z∂x)2∂2z∂y2=0. \begin{align} & \left(\dfrac {\partial z}{\partial y}\right)^{2}\dfrac {\partial ^{2}z}{\partial x^{2}}-2\dfrac {\partial z}{\partial x}\dfrac {\partial z}{\partial y}\dfrac {\partial ^{2}z}{\partial x \partial y} \\ & \quad +\left(\dfrac {\partial z}{\partial x}\right)^{2}\dfrac {\partial ^{2}z}{\partial y^{2}}=0 . \end{align}
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Problem 3527

Using the Legendre transform

X=∂z∂x,Y=∂z∂y,Z=x∂z∂x+y∂z∂y−z, X=\dfrac {\partial z}{\partial x} , \quad Y=\dfrac {\partial z}{\partial y} , \quad Z=x\dfrac {\partial z}{\partial x}+y\dfrac {\partial z}{\partial y}-z ,

where Z=Z(X,Y)Z=Z(X,Y), transform the equation

A(∂z∂x,∂z∂y)∂2z∂x2+2B(∂z∂x,∂z∂y)∂2z∂x∂y+C(∂z∂x,∂z∂y)∂2z∂y2=0. \begin{align} & A\left(\dfrac {\partial z}{\partial x}, \dfrac {\partial z}{\partial y}\right)\dfrac {\partial ^{2}z}{\partial x^{2}}+2B\left(\dfrac {\partial z}{\partial x}, \dfrac {\partial z}{\partial y}\right)\dfrac {\partial ^{2}z}{\partial x \partial y} \\ & \quad +C\left(\dfrac {\partial z}{\partial x}, \dfrac {\partial z}{\partial y}\right)\dfrac {\partial ^{2}z}{\partial y^{2}}=0 . \end{align}
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