Section 3.7

Functions of Several Variables. Their Derivatives and Differentials

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Problem 1199

Show that

lim⁡y→0lim⁡x→0x2−y2x2+y2=−1,lim⁡x→0lim⁡y→0x2−y2x2+y2=1. \lim _{y \to 0} \lim _{x \to 0} \frac{x^{2}-y^{2}}{x^{2}+y^{2}} = -1, \qquad \lim _{x \to 0} \lim _{y \to 0} \frac{x^{2}-y^{2}}{x^{2}+y^{2}} = 1.
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Problem 1200

Show that

lim⁡x→∞lim⁡y→∞x2+y21+(x−y)4=lim⁡y→∞lim⁡x→∞x2+y21+(x−y)4, \lim _{x \to \infty } \lim _{y \to \infty } \frac{x^{2}+y^{2}}{1+(x-y)^{4}} = \lim _{y \to \infty } \lim _{x \to \infty } \frac{x^{2}+y^{2}}{1+(x-y)^{4}},

while the quantity

lim⁡x,y→∞x2+y21+(x−y)4 \lim _{x,y \to \infty } \frac{x^{2}+y^{2}}{1+(x-y)^{4}}

nevertheless has no meaning.

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Problem 1201

Show that if x→∞x \to \infty and y→∞y \to \infty in such a way that the ratio yx\frac{y}{x} has any given constant value, then 11+(x2−y)→0\frac{1}{1+(x^{2}-y)} \to 0. At the same time, this quantity may fail to tend to any limit if the ratio yx\frac{y}{x} is not constant.

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Problem 1202

Show that f(x)f(x), defined by the equality

f(x)=lim⁡n→∞lim⁡m→∞cos⁡mn! 2πx, f(x) = \lim _{n \to \infty } \lim _{m \to \infty } \cos ^{m} n! \, 2\pi x,

equals one if xx is a rational number, and zero if xx is an irrational number; mm and nn are natural numbers.

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Problem 1203

Show that in any neighborhood of the point (0,0)(0,0) the function f(x,y)f(x,y), defined by the equalities

f(0,0)=0,f(x,y)=x2−y2x2+y2for x2+y2>0, f(0,0) = 0, \qquad f(x,y) = \frac{x^{2}-y^{2}}{x^{2}+y^{2}} \quad \text{for } x^{2}+y^{2} > 0,

takes every value in the interval (−1,1)(-1,1). Here, by a neighborhood of the point (0,0)(0,0) is meant any region (a disk, a rectangle, etc.) containing the point (0,0)(0,0) in its interior.

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Problem 1204

A function is defined by the equalities:

f(x,y)=xyx2+y2for x2+y2>0,f(0,0)=0. f(x,y) = \frac{xy}{x^{2}+y^{2}} \quad \text{for } x^{2}+y^{2} > 0, \qquad f(0,0) = 0.

Show that this function is continuous with respect to each of the variables xx and yy separately, without being, in a neighborhood of the point (0,0)(0,0), a continuous function of both variables under their joint variation.

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Problem 1205

Show that the function, defined for x2+y2>0x^{2}+y^{2} > 0 by the equality f(x,y)=ex/(x2+y2)f(x,y) = e^{x/(x^{2}+y^{2})}, takes every positive value in any region containing the point (0,0)(0,0) in its interior.

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Problem 1206

Find the partial derivatives of the function u=x3+y3−3xyu = x^{3}+y^{3}-3xy.

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Problem 1207

Find the partial derivatives of the function u=2x3−3x2y2+3y3u = 2x^{3}-3x^{2}y^{2}+3y^{3}.

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Problem 1208

Find the partial derivatives of the function u=xy+xz+yzu = xy+xz+yz.

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Problem 1209

Find the partial derivatives of the function u=xyu = x^{y}.

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Problem 1210

Find the partial derivatives of the function u=x3+yz2+3xy−x+zu = x^{3}+yz^{2}+3xy-x+z.

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Problem 1211

Find the partial derivatives of the function u=exyu = e^{xy}.

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Problem 1212

Find the partial derivatives of the function u=arctg⁡xyu = \operatorname {arctg} \frac{x}{y}.

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Problem 1213

Find the partial derivatives of the function u=xy−3x+5yu = xy-\frac{3}{x}+\frac{5}{y}.

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Problem 1214

Find the partial derivatives of the function u=x2+y2+z2+xy+xz+yzu = x^{2}+y^{2}+z^{2}+xy+xz+yz.

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Problem 1215

Find the partial derivatives of the function u=(xy)zu = (xy)^{z}.

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Problem 1216

Find the partial derivatives of the function u=zxyu = z^{xy}.

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Problem 1217

Find the total differential of the function u=sin⁡(x2+y2)u = \sin (x^{2}+y^{2}).

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Problem 1218

Find the total differential of the function u=arctg⁡xyu = \operatorname {arctg} \frac{x}{y}.

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Problem 1219

Find the total differential of the function u=ln⁡tg⁡xyu = \ln \operatorname {tg} \frac{x}{y}.

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Problem 1220

Find the total differential of the function u=x2+y2+z2u = \sqrt{x^{2}+y^{2}+z^{2}}.

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Problem 1221

Find the total differential of the function u=ln⁡(x+y+z)u = \ln (x+y+z).

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Problem 1222

Find the total differential of the function u=xyu = x^{y}.

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Problem 1223

Verify Euler's theorem on an example by direct computation of the derivatives: u=x2+y2+z2ln⁡xyu = \sqrt{x^{2}+y^{2}+z^{2}} \ln \frac{x}{y}.

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Remark.
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If, when all the variables are increased tt-fold, a function is multiplied by tnt^{n}, then it is called a homogeneous function of degree nn. Thus, for example, if

f(tx,ty,tz)=tnf(x,y,z), f(tx,ty,tz) = t^{n}f(x,y,z),

then f(x,y,z)f(x,y,z) is a homogeneous function of degree nn. By Euler's theorem, if f(x1,x2,…,xm)f(x_{1},x_{2},\ldots ,x_{m}) is a homogeneous function of degree nn, then the equality

x1∂f∂x1+x2∂f∂x2+…+xm∂f∂xm=nf(x1,x2,…,xm). x_{1}\frac{\partial f}{\partial x_{1}}+x_{2}\frac{\partial f}{\partial x_{2}}+\ldots +x_{m}\frac{\partial f}{\partial x_{m}} = nf(x_{1},x_{2},\ldots ,x_{m}).

holds.

Problem 1224

Verify Euler's theorem by direct computation of the derivatives: u=xyex/zu = \frac{x}{y}e^{x/z}.

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Problem 1225

Verify Euler's theorem by direct computation of the derivatives: u=sin⁡x+y+zx2+y2+z2u = \sin \frac{x+y+z}{\sqrt{x^{2}+y^{2}+z^{2}}}.

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Problem 1226

Verify Euler's theorem by direct computation of the derivatives: u=xx2+y2+z2u = \frac{x}{x^{2}+y^{2}+z^{2}}.

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Problem 1227

Verify Euler's theorem by direct computation of the derivatives: u=x2+y2+z2u = \sqrt{x^{2}+y^{2}+z^{2}}.

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Problem 1228

Verify Euler's theorem by direct computation of the derivatives: u=arctg⁡xyu = \operatorname {arctg} \frac{x}{y}.

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Problem 1229

Find the derivative of the function f=4x3−2xy+3y3f = 4x^{3}-2xy+3y^{3} at the point (1,2)(1,2) in the direction π3\frac{\pi }{3} to the OxOx axis.

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Problem 1230

Find the derivative of the function f=5x+10x2y+y5f = 5x+10x^{2}y+y^{5} at the point (1,2)(1,2) in the direction toward the point (5,−1)(5,-1).

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Problem 1231

Find the derivative of the function f=x2+y2f = x^{2}+y^{2} at the point (1,2)(1,2) in the direction of the line 3x+4y=113x+4y = 11:

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(a)

in the direction of increasing xx;

(b)

in the direction of decreasing xx.

Problem 1232

Write the expression for the derivative of the function f(x,y)f(x,y):

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(a)

in the direction of the tangent to the curve φ(x,y)=C\varphi (x,y) = C;

(b)

in the direction of the normal to the curve φ(x,y)=C\varphi (x,y) = C.

Problem 1233

Find the derivative of the function f=x3+2xy2+3yz2f = x^{3}+2xy^{2}+3yz^{2} at the point (3,3,1)(3,3,1) in the direction of the vector 2i→+2j→+k→2\overrightarrow {i}+2\overrightarrow {j}+\overrightarrow {k}.

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Problem 1234

Find the derivative of the function F=x2a2+y2b2+z2c2F = \frac{x^{2}}{a^{2}}+\frac{y^{2}}{b^{2}}+\frac{z^{2}}{c^{2}} in the direction of the outward normal to the surface F=constF = \mathrm{const}.

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Problem 1235

Find ∂2u∂x2\frac{\partial^{2} u}{\partial x^{2}}, ∂2u∂x∂y\frac{\partial^{2} u}{\partial x \partial y}, ∂2u∂y2\frac{\partial^{2} u}{\partial y^{2}}; u=12ln⁡(x2+y2)u = \frac{1}{2}\ln (x^{2}+y^{2}).

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Problem 1236

Find ∂2u∂x2\frac{\partial^{2} u}{\partial x^{2}}, ∂2u∂x∂y\frac{\partial^{2} u}{\partial x \partial y}, ∂2u∂y2\frac{\partial^{2} u}{\partial y^{2}}; u=arctg⁡x+y1−xyu = \operatorname {arctg} \frac{x+y}{1-xy}.

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Problem 1237

Find ∂2u∂x2\frac{\partial^{2} u}{\partial x^{2}}, ∂2u∂x∂y\frac{\partial^{2} u}{\partial x \partial y}, ∂2u∂y2\frac{\partial^{2} u}{\partial y^{2}}; u=xsin⁡(x+y)+ycos⁡(x+y)u = x\sin (x+y)+y\cos (x+y).

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Problem 1238

Find ∂2u∂x∂y\frac{\partial^{2} u}{\partial x \partial y}, if u=xyu = x^{y}.

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Problem 1239

Find ∂3u∂x2∂y\frac{\partial^{3} u}{\partial x^{2} \partial y}, if u=ln⁡(x+y)u = \ln (x+y).

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Problem 1240

Find ∂4u∂x2∂y2\frac{\partial^{4} u}{\partial x^{2} \partial y^{2}}, if u=ln⁡(x2+y2)u = \ln (x^{2}+y^{2}).

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Problem 1241

Find ∂2u∂x2\frac{\partial^{2} u}{\partial x^{2}}, ∂2u∂y2\frac{\partial^{2} u}{\partial y^{2}}, ∂2u∂z2\frac{\partial^{2} u}{\partial z^{2}}, if u=x2+y2+z2u = \sqrt{x^{2}+y^{2}+z^{2}}.

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Problem 1242

Find ∂3u∂x∂y∂z\frac{\partial^{3} u}{\partial x \partial y \partial z}, if u=exyzu = e^{xyz}.

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Problem 1243

Find d2ud^{2}u, if u=x2−xy+2y2+3x−5y+7u = x^{2}-xy+2y^{2}+3x-5y+7.

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Problem 1244

Find d2ud^{2}u, if u=x2y2u = x^{2}y^{2}.

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Problem 1245

Find d2ud^{2}u, if u=exyu = e^{xy}.

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Problem 1246

Find d2ud^{2}u, if u=12ln⁡(x2+y2)u = \frac{1}{2}\ln (x^{2}+y^{2}).

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Problem 1247

Find d2ud^{2}u, if u=sin⁡(x+y+z)u = \sin (x+y+z).

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Problem 1248

Find d4ud^{4}u, if u=x4+4x3y+2xy2z−3xyz2+z4u = x^{4}+4x^{3}y+2xy^{2}z-3xyz^{2}+z^{4}.

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Problem 1249

Find d4ud^{4}u, if u=x4−3x2y2+y4+5xyz−x3−y3+x2−xy+y2+2x−5yu = x^{4}-3x^{2}y^{2}+y^{4}+5xyz-x^{3}-y^{3}+x^{2}-xy+y^{2}+2x-5y.

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Problem 1250

Find d4ud^{4}u, if u=x4+3x3y+z4−x2y+z3u = x^{4}+3x^{3}y+z^{4}-x^{2}y+z^{3}.

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Problem 1251

Find d3ud^{3}u, if u=xyzu = xyz.

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Problem 1252

Find d4ud^{4}u, if u=ln⁡(2x+3y−z)u = \ln (2x+3y-z).

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Problem 1253

Find the partial derivatives by first computing the total differentials of the needed order: u=sin⁡(2x+y)u = \sin (2x+y); find ∂3u∂x3\frac{\partial^{3} u}{\partial x^{3}} and ∂3u∂x∂y2\frac{\partial^{3} u}{\partial x \partial y^{2}}.

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Problem 1254

Find the partial derivatives by first computing the total differentials of the needed order: u=cos⁡(x+y)u = \cos (x+y); find ∂4u∂x2∂y2\frac{\partial^{4} u}{\partial x^{2} \partial y^{2}}.

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Problem 1255

Find the partial derivatives by first computing the total differentials of the needed order: u=ln⁡(ax+by+cz)u = \ln (ax+by+cz); find ∂4u∂x4\frac{\partial^{4} u}{\partial x^{4}} and ∂4u∂x2∂y2\frac{\partial^{4} u}{\partial x^{2} \partial y^{2}}.

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Problem 1256

Find the partial derivatives by first computing the total differentials of the needed order: u=ex+2y+3zu = e^{x+2y+3z}; find ∂3u∂x3\frac{\partial^{3} u}{\partial x^{3}} and ∂3u∂x∂y∂z\frac{\partial^{3} u}{\partial x \partial y \partial z}.

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Problem 1257

Find the total differentials of the first two orders for the composite function u=φ(t)u = \varphi (t); t=xyt = xy.

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Problem 1258

Find the total differentials of the first two orders for the composite function u=φ(t)u = \varphi (t); t=x2+y2t = x^{2}+y^{2}.

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Problem 1259

Find the total differentials of the first two orders for the composite function u=φ(t)u = \varphi (t); t=x2+y2+z2t = x^{2}+y^{2}+z^{2}.

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Problem 1260

Find the total differentials of the first two orders for the composite function u=φ(ξ,η)u = \varphi (\xi ,\eta ); ξ=ax+by+cz\xi = ax+by+cz, η=a1x+b1y+c1z\eta = a_{1}x+b_{1}y+c_{1}z.

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Problem 1261

Find the total differentials of the first two orders for the composite function u=φ(ξ,η,ζ)u = \varphi (\xi ,\eta ,\zeta ); ξ=ax\xi = ax, η=by\eta = by, ζ=cz\zeta = cz.

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Problem 1262

Find the derivatives of the first two orders of the function u=φ(ξ,η)u = \varphi (\xi ,\eta ); ξ=x+y\xi = x+y, η=x−y\eta = x-y.

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Problem 1263

Find the derivatives of the first two orders of the function u=φ(ξ,η)u = \varphi (\xi ,\eta ); ξ=x2+y2\xi = x^{2}+y^{2}, η=xy\eta = xy.

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Problem 1264

Find the derivatives of order nn of u=φ(t)u = \varphi (t), where t=ax+by+czt = ax+by+cz.

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Problem 1265

Find ∂nu∂xn\frac{\partial^{n} u}{\partial x^{n}}, if u=φ(ξ,η,ζ)u = \varphi (\xi ,\eta ,\zeta ), ξ=ax\xi = ax, η=by\eta = by, ζ=cz\zeta = cz.

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Problem 1266

Show that if x2=ηξx^{2} = \eta \xi, y2=ζξy^{2} = \zeta \xi, z2=ξηz^{2} = \xi \eta, then

x∂u∂x+y∂u∂y+z∂u∂z=ξ∂u∂ξ+η∂u∂η+ζ∂u∂ζ. x\frac{\partial u}{\partial x}+y\frac{\partial u}{\partial y}+z\frac{\partial u}{\partial z} = \xi \frac{\partial u}{\partial \xi }+\eta \frac{\partial u}{\partial \eta }+\zeta \frac{\partial u}{\partial \zeta }.
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Problem 1267

Setting x=ρcos⁡φx = \rho \cos \varphi, y=ρsin⁡φy = \rho \sin \varphi, find

∣∂x∂ρ∂x∂φ∂y∂ρ∂y∂φ∣. \begin{vmatrix} \frac{\partial x}{\partial \rho } & \frac{\partial x}{\partial \varphi } \\ \frac{\partial y}{\partial \rho } & \frac{\partial y}{\partial \varphi } \end{vmatrix}.
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Problem 1268

Setting x=ρsin⁡φcos⁡ψx = \rho \sin \varphi \cos \psi, y=ρsin⁡φsin⁡ψy = \rho \sin \varphi \sin \psi, z=ρcos⁡φz = \rho \cos \varphi, compute the value of the functional determinant (Jacobian)

D(x,y,z)D(ρ,φ,ψ)=∣∂x∂ρ∂x∂φ∂x∂ψ∂y∂ρ∂y∂φ∂y∂ψ∂z∂ρ∂z∂φ∂z∂ψ∣. \frac{D(x,y,z)}{D(\rho ,\varphi ,\psi )} = \begin{vmatrix} \frac{\partial x}{\partial \rho } & \frac{\partial x}{\partial \varphi } & \frac{\partial x}{\partial \psi } \\ \frac{\partial y}{\partial \rho } & \frac{\partial y}{\partial \varphi } & \frac{\partial y}{\partial \psi } \\ \frac{\partial z}{\partial \rho } & \frac{\partial z}{\partial \varphi } & \frac{\partial z}{\partial \psi } \end{vmatrix}.
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Problem 1269

Setting r2=a2+ρ2−2aρcos⁡φr^{2} = a^{2}+\rho^{2}-2a\rho \cos \varphi, find D(ρ,φ,ψ)D(ρ,r,ψ)\frac{D(\rho ,\varphi ,\psi )}{D(\rho ,r,\psi )}.

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Problem 1270

Setting x=ξηζx = \xi \eta \zeta, y=ξη−ξηζy = \xi \eta -\xi \eta \zeta, z=η−ξηz = \eta -\xi \eta, find the Jacobian D(x,y,z)D(ξ,η,ζ)\frac{D(x,y,z)}{D(\xi ,\eta ,\zeta )}.

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Problem 1271

Prove that for x=cos⁡φx = \cos \varphi, y=sin⁡φcos⁡θy = \sin \varphi \cos \theta, z=sin⁡φsin⁡θcos⁡ψz = \sin \varphi \sin \theta \cos \psi the Jacobian equals −sin⁡3φsin⁡2θsin⁡ψ-\sin^{3}\varphi \sin^{2}\theta \sin \psi.

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Problem 1272

Prove that for

u1=x11−r2,u2=x21−r2,u3=x31−r2, u_{1} = \frac{x_{1}}{\sqrt{1-r^{2}}}, \qquad u_{2} = \frac{x_{2}}{\sqrt{1-r^{2}}}, \qquad u_{3} = \frac{x_{3}}{\sqrt{1-r^{2}}},

where r2=x12+x22+x32r^{2} = x_{1}^{2}+x_{2}^{2}+x_{3}^{2}; the equality

D(u1,u2,u3)D(x1,x2,x3)=(1−r2)−5/2. \frac{D(u_{1},u_{2},u_{3})}{D(x_{1},x_{2},x_{3})} = (1-r^{2})^{-5/2}.

holds.

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Problem 1273

Prove that

D(∂v∂x1,∂v∂x2,…,∂v∂xn)D(y1,y2,…,yn)=D(∂v∂y1,∂v∂y2,…,∂v∂yn)D(x1,x2,…,xn). \frac{D\left(\frac{\partial v}{\partial x_{1}},\frac{\partial v}{\partial x_{2}},\ldots ,\frac{\partial v}{\partial x_{n}}\right)}{D(y_{1},y_{2},\ldots ,y_{n})} = \frac{D\left(\frac{\partial v}{\partial y_{1}},\frac{\partial v}{\partial y_{2}},\ldots ,\frac{\partial v}{\partial y_{n}}\right)}{D(x_{1},x_{2},\ldots ,x_{n})}.

Here v=v(x1,x2,…,xn;y1,y2,…,yn)v = v(x^{1},x^{2},\ldots ,x_{n};y^{1},y_{2},\ldots ,y_{n}) is a function with continuous second derivatives.

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Problem 1274

Prove that for homogeneous functions φ(x,y,z)\varphi (x,y,z) of degree nn the equality

(x∂∂x+y∂∂y+z∂∂z)mφ=n(n−1)…(n−m+1)φ. \left(x\frac{\partial }{\partial x}+y\frac{\partial }{\partial y}+z\frac{\partial }{\partial z}\right)^{m} \varphi = n(n-1) \ldots (n-m+1)\varphi .

holds.

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Problem 1275

Verify that ∂u∂t=a2∂2u∂x2\frac{\partial u}{\partial t} = a^{2}\frac{\partial^{2} u}{\partial x^{2}}, if u=1te−x2/(4a2t)u = \frac{1}{\sqrt{t}} e^{-x^{2}/(4a^{2}t)}.

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Problem 1276

Verify that x∂u∂x+y∂u∂y+z∂u∂z=0x\frac{\partial u}{\partial x}+y\frac{\partial u}{\partial y}+z\frac{\partial u}{\partial z} = 0, if u=(xy)z/yu = \left(\frac{x}{y}\right)^{z/y}.

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Problem 1277

Compute ∂2u∂x2−2∂2u∂x∂y+∂2u∂y2\frac{\partial^{2} u}{\partial x^{2}}-2\frac{\partial^{2} u}{\partial x \partial y}+\frac{\partial^{2} u}{\partial y^{2}}, if u=φ(x+y)u = \varphi (x+y).

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Problem 1278

Compute x2∂2u∂x2−2xy∂2u∂x∂y+y2∂2u∂y2x^{2}\frac{\partial^{2} u}{\partial x^{2}}-2xy\frac{\partial^{2} u}{\partial x \partial y}+y^{2}\frac{\partial^{2} u}{\partial y^{2}}, if u=f(x2+y2)u = f\left(\sqrt{x^{2}+y^{2}}\right).

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Problem 1279

Compute ∂2u∂x2⋅∂2u∂y2−(∂2u∂x∂y)2\frac{\partial^{2} u}{\partial x^{2}} \cdot \frac{\partial^{2} u}{\partial y^{2}}-\left(\frac{\partial^{2} u}{\partial x \partial y}\right)^{2}, if u=φ(xy)u = \varphi (xy).

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Problem 1280

The function called the potential of the ball x2+y2+z2=a2x^{2}+y^{2}+z^{2} = a^{2} is defined by the equalities:

u={2πa2−2π3(x2+y2+z2),for x2+y2+z2<a2;4πa33x2+y2+z2,for x2+y2+z2≥a2. u = \begin{cases} 2\pi a^{2}-\frac{2\pi }{3}(x^{2}+y^{2}+z^{2}), & \text{for } x^{2}+y^{2}+z^{2} < a^{2}; \\ \frac{4\pi a^{3}}{3\sqrt{x^{2}+y^{2}+z^{2}}}, & \text{for } x^{2}+y^{2}+z^{2} \geq a^{2}. \end{cases}

Verify that uu and its first derivatives are continuous for any xx, yy, and zz, and that the Laplacian

Δu=∂2u∂x2+∂2u∂y2+∂2u∂z2=0or −4π, \Delta u = \frac{\partial ^{2} u}{\partial x^{2}}+\frac{\partial ^{2} u}{\partial y^{2}}+\frac{\partial ^{2} u}{\partial z^{2}} = 0 \quad \text{or } -4\pi ,

depending on whether the point M(x,y,z)M(x,y,z) lies outside the ball x2+y2+z2=a2x^{2}+y^{2}+z^{2} = a^{2} or inside it.

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Problem 1281

Verify the equality

(x∂∂x+y∂∂y+z∂∂z)2u=0,u=x2+y2+z2. \left(x\frac{\partial }{\partial x}+y\frac{\partial }{\partial y}+z\frac{\partial }{\partial z}\right)^{2} u = 0, \qquad u = \sqrt{x^{2}+y^{2}+z^{2}}.
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Problem 1282

Verify the equality ∂u∂x+∂u∂y+∂u∂z=3x+y+z\frac{\partial u}{\partial x}+\frac{\partial u}{\partial y}+\frac{\partial u}{\partial z} = \frac{3}{x+y+z}; u=ln⁡(x3+y3+z3−3xyz)u = \ln (x^{3}+y^{3}+z^{3}-3xyz).

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Problem 1283

Verify the equality 1x∂z∂x+1y∂z∂y=zy2\frac{1}{x}\frac{\partial z}{\partial x}+\frac{1}{y}\frac{\partial z}{\partial y} = \frac{z}{y^{2}}; z=yφ(x2−y2)z = y\varphi (x^{2}-y^{2}).

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Problem 1284

Verify the equality x∂u∂x+y∂u∂y=xy+ux\frac{\partial u}{\partial x}+y\frac{\partial u}{\partial y} = xy+u; u=xy+xφ(yx)u = xy+x\varphi \left(\frac{y}{x}\right).

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Problem 1285

Verify the equality ∂2ln⁡r∂x2+∂2ln⁡r∂y2+∂2ln⁡r∂z2=1r2\frac{\partial^{2} \ln r}{\partial x^{2}}+\frac{\partial^{2} \ln r}{\partial y^{2}}+\frac{\partial^{2} \ln r}{\partial z^{2}} = \frac{1}{r^{2}}; r=x2+y2+z2r = \sqrt{x^{2}+y^{2}+z^{2}}.

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Problem 1286

Verify the equality ∂2u∂x2−∂2u∂y2−2α∂u∂y=α2u\frac{\partial^{2} u}{\partial x^{2}}-\frac{\partial^{2} u}{\partial y^{2}}-2\alpha \frac{\partial u}{\partial y} = \alpha^{2}u; u=e−αxφ(x−y)u = e^{-\alpha x}\varphi (x-y).

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Problem 1287

Verify the equality ∂2u∂x2−∂2u∂y2=−2φ′′\frac{\partial^{2} u}{\partial x^{2}}-\frac{\partial^{2} u}{\partial y^{2}} = -2\varphi ''; u=φ(y−x)−xφ′(y−x)u = \varphi (y-x)-x\varphi '(y-x).

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Problem 1288

Verify the equality (x2−y2)∂z∂x+xy∂z∂y=xyz(x^{2}-y^{2})\frac{\partial z}{\partial x}+xy\frac{\partial z}{\partial y} = xyz; z=eyφ(yex2/(2y2))z = e^{y}\varphi \left(ye^{x^{2}/(2y^{2})}\right).

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Problem 1289

Verify the equality x∂u∂x+y∂u∂y=u−x2−y2x\frac{\partial u}{\partial x}+y\frac{\partial u}{\partial y} = u-x^{2}-y^{2}; u=xφ(yx)−x2−y2u = x\varphi \left(\frac{y}{x}\right)-x^{2}-y^{2}.

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Problem 1290

Verify the equality ∂2u∂t2=a2∂2u∂x2\frac{\partial^{2} u}{\partial t^{2}} = a^{2}\frac{\partial^{2} u}{\partial x^{2}}; u=φ(x+at)+ψ(x−at)u = \varphi (x+at)+\psi (x-at).

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Problem 1291

Verify the equality ∂2u∂x2+∂2u∂y2=0\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}} = 0; u=ln⁡(x2+y2)u = \ln (x^{2}+y^{2}).

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Problem 1292

Verify the equality ∂2u∂x2+∂2u∂y2+∂2u∂z2=0\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}+\frac{\partial^{2} u}{\partial z^{2}} = 0; u=1x2+y2+z2u = \frac{1}{\sqrt{x^{2}+y^{2}+z^{2}}}.

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Problem 1293

Verify the equality ∂2u∂x2+∂2u∂y2+∂2u∂z2=a2u\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}+\frac{\partial^{2} u}{\partial z^{2}} = a^{2}u; u=1r(Ae−ar+Bear)u = \frac{1}{r}(Ae^{-ar}+Be^{ar}), where r=x2+y2+z2r = \sqrt{x^{2}+y^{2}+z^{2}}.

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Problem 1294

Verify the equality ∂2ln⁡z∂x∂y=2z\frac{\partial^{2} \ln z}{\partial x \partial y} = 2z; z=φ′(x)ψ′(x)(φ(x)+ψ(y))2z = \frac{\varphi '(x)\psi '(x)}{(\varphi (x)+\psi (y))^{2}}.

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Problem 1295

Verify the equality x2∂2u∂x2+2xy∂2u∂x∂y+y2∂2u∂y2=0x^{2}\frac{\partial^{2} u}{\partial x^{2}}+2xy\frac{\partial^{2} u}{\partial x \partial y}+y^{2}\frac{\partial^{2} u}{\partial y^{2}} = 0, if u=xφ(yx)u = x\varphi \left(\frac{y}{x}\right).

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Problem 1296

Verify the equality x2∂2u∂x2+2xy∂2u∂x∂y+y2∂2u∂y2+x∂u∂x+y∂u∂y=n2ux^{2}\frac{\partial^{2} u}{\partial x^{2}}+2xy\frac{\partial^{2} u}{\partial x \partial y}+y^{2}\frac{\partial^{2} u}{\partial y^{2}}+x\frac{\partial u}{\partial x}+y\frac{\partial u}{\partial y} = n^{2}u, where u=xnφ(yx)+y−nψ(yx)u = x^{n}\varphi \left(\frac{y}{x}\right)+y^{-n}\psi \left(\frac{y}{x}\right).

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Problem 1297

Verify the equality x2∂2u∂x2+2xy∂2u∂x∂y+y2∂2u∂y2=n(n−1)ux^{2}\frac{\partial^{2} u}{\partial x^{2}}+2xy\frac{\partial^{2} u}{\partial x \partial y}+y^{2}\frac{\partial^{2} u}{\partial y^{2}} = n(n-1)u, where u=xnφ(yx)+x1−nψ(yx)u = x^{n}\varphi \left(\frac{y}{x}\right)+x^{1-n}\psi \left(\frac{y}{x}\right).

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Problem 1298

Verify the equality ∂u∂x⋅∂2u∂x∂y=∂u∂y⋅∂2u∂x2\frac{\partial u}{\partial x} \cdot \frac{\partial^{2} u}{\partial x \partial y} = \frac{\partial u}{\partial y} \cdot \frac{\partial^{2} u}{\partial x^{2}}, if u=f(x+φ(y))u = f\left(x+\varphi (y)\right).

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Problem 1299

Verify the equality ∂2u∂x2−2∂2u∂x∂y+∂2u∂y2=0\frac{\partial^{2} u}{\partial x^{2}}-2\frac{\partial^{2} u}{\partial x \partial y}+\frac{\partial^{2} u}{\partial y^{2}} = 0, if u=xφ(x+y)+yψ(x+y)u = x\varphi (x+y)+y\psi (x+y).

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Problem 1300

Verify the equality

a2(u∂2u∂x2−(∂u∂x)2)=b2(u∂2u∂y2−(∂u∂y)2), a^{2}\left(u\frac{\partial ^{2} u}{\partial x^{2}}-\left(\frac{\partial u}{\partial x}\right)^{2}\right) = b^{2}\left(u\frac{\partial ^{2} u}{\partial y^{2}}-\left(\frac{\partial u}{\partial y}\right)^{2}\right),

where u=φ(ay+bx)ψ(bx−ay)u = \varphi (ay+bx)\psi (bx-ay).

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