Section 2.5

Second-Order Surfaces. Center and Diametral Planes

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Problem 555

Find the general equation of second-order surfaces cut by the plane xOyxOy in the curve αx2+βxy+γy2+δx+εy+ζ=0\alpha x^{2}+\beta xy+\gamma y^{2}+\delta x+\varepsilon y+\zeta = 0.

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Problem 556

Find the second-order surface on which lie the circles

{z=0,x2+y2−1=0,{z=1,x2+y2−3=0,{z=2,x2+y2−5=0. \begin{cases} z = 0, \\ x^{2}+y^{2}-1 = 0, \end{cases} \qquad \begin{cases} z = 1, \\ x^{2}+y^{2}-3 = 0, \end{cases} \qquad \begin{cases} z = 2, \\ x^{2}+y^{2}-5 = 0. \end{cases}
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Problem 557

Through the origin draw lines of asymptotic direction for the surface x2−2y2−4xy−10xz−4yz−10=0x^{2}-2y^{2}-4xy-10xz-4yz-10 = 0, parallel to the plane 3x+y−4z−3=03x+y-4z-3 = 0.

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Problem 558

Show that the equation x2+y2+z2+2xz+2y+1=0x^{2}+y^{2}+z^{2}+2xz+2y+1 = 0 is satisfied only by the points of the line

{x+z=0,y+1=0. \begin{cases} x+z = 0, \\ y+1 = 0. \end{cases}
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Problem 559

Show that the equation

3x2+3y2+3z2+2xy+2xz−2yz+2x−2y−2z+3=0 3x^{2}+3y^{2}+3z^{2}+2xy+2xz-2yz+2x-2y-2z+3 = 0

is satisfied by the coordinates of only one point (−1,1,1)(-1,1,1).

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Problem 560

Write a second-order equation that is satisfied only by the coordinates of the point (2,1,1)(2,1,1).

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Problem 561

Set up a second-order equation that is satisfied only by the coordinates of the points of the line 2x+2=3y=2z2x+2 = 3y = 2z.

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Problem 562

Find the equation of the pair of planes x+2y−z+1=0x+2y-z+1 = 0 and x−y+z+1=0x-y+z+1 = 0.

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Problem 563

Find the lines along which the conical surface z2−2xy−4x−2y+2z−3=0z^{2}-2xy-4x-2y+2z-3 = 0 intersects the plane x+y+2z+5=0x+y+2z+5 = 0.

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Problem 564

Find the generators of the surface x2+y2−z2=1x^{2}+y^{2}-z^{2} = 1 passing through the point (1,1,1)(1,1,1).

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Problem 565

Find the generator of the surface x2−y2=2zx^{2}-y^{2} = 2z parallel to the plane x+y+z=0x+y+z = 0.

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Problem 566

Find the lines parallel to the generators of the two surfaces:

x2a2+y2b2−z2c2=1andy2p−z2q=2x. \frac{x^{2}}{a^{2}}+\frac{y^{2}}{b^{2}}-\frac{z^{2}}{c^{2}} = 1 \qquad \text{and} \qquad \frac{y^{2}}{p}-\frac{z^{2}}{q} = 2x.
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Problem 567

Through the points (0,−2,2)(0,-2,2) and (−1,0,0)(-1,0,0) draw planes intersecting the cone x2+y2=z2x^{2}+y^{2} = z^{2} in parabolas.

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Problem 568

Through the same points draw planes intersecting the same cone in ellipses.

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Problem 569

Transform the equation x2+y2+z2+2xy−2yz+6xz+2x−6y−2z=0x^{2}+y^{2}+z^{2}+2xy-2yz+6xz+2x-6y-2z = 0 by moving the origin to the center.

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Problem 570

The same for the surface

2x2+6y2+2z2+8xz−4x−8y+3=0. 2x^{2}+6y^{2}+2z^{2}+8xz-4x-8y+3 = 0.
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Problem 571

The same for the surface 4xy+4xz−4y−4z−1=04xy+4xz-4y-4z-1 = 0.

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Problem 572

Find the locus of the centers of the surfaces x2+y2−z2+λxz+μyz−2x−2y−2z=0x^{2}+y^{2}-z^{2}+\lambda xz+\mu yz-2x-2y-2z = 0.

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Problem 573

From the center of the surface x2+4y2−40z2+4x−8y−16z−12=0x^{2}+4y^{2}-40z^{2}+4x-8y-16z-12 = 0 draw lines of asymptotic direction.

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Problem 574

Find the equation of the hyperboloid passing through the point (2,1,1)(2,1,1), given the asymptotic cone of this hyperboloid x2+y2−z2=0x^{2}+y^{2}-z^{2} = 0.

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Problem 575

Prove that the locus of the centers of second-order surfaces passing through a given ellipse and through two points symmetric with respect to the plane of this ellipse is a second-order surface.

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Problem 576

Denoting by sλμνs_{\lambda \mu \nu } the left-hand side of the equation of the plane passing through the points λ\lambda and μ\mu, prove that the equation

s123s456+As234s561+Bs345s612+Cs124s356=0 s_{123}s_{456}+As_{234}s_{561}+Bs_{345}s_{612}+Cs_{124}s_{356} = 0

for any choice of the coefficients AA, BB, and CC represents a second-order surface passing through the six given points labeled 1,2,3,4,51,2,3,4,5, and 66.

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Problem 577

The general equation of a second-order surface can be written in the form Ax2+By2+Cz2+Dxy+Exz+Fyz+Gx+Hy+Iz+K=0Ax^{2}+By^{2}+Cz^{2}+Dxy+Exz+Fyz+Gx+Hy+Iz+K = 0. By introducing a variable tt, the left-hand side can be turned into a quadratic form in four variables

Φ(x,y,z,t)=Ax2+By2+Cz2+Dxy+Exz+Fyz+Gxt+Hyt+Izt+Kt2, \Phi (x,y,z,t) = Ax^{2}+By^{2}+Cz^{2}+Dxy+Exz+Fyz+Gxt+Hyt+Izt+Kt^{2},

so that at t=1t = 1 the equation of the surface is written as Φ(x,y,z,1)=0\Phi (x,y,z,1) = 0. At t=0t = 0 the form Φ\Phi becomes the ternary quadratic form f(x,y,z)=Ax2+By2+Cz2+Dxy+Exz+Fyzf(x,y,z) = Ax^{2}+By^{2}+Cz^{2}+Dxy+Exz+Fyz. The following identity holds (the Taylor formula for a quadratic form):

Φ(x+ξ,y+η,z+ζ,t+τ)=Φ(x,y,z,t)+∂Φ∂xξ+∂Φ∂yη+∂Φ∂zζ+∂Φ∂tτ+Φ(ξ,η,ζ,τ).(*) \Phi (x+\xi ,y+\eta ,z+\zeta ,t+\tau ) = \Phi (x,y,z,t)+\frac{\partial \Phi }{\partial x}\xi +\frac{\partial \Phi }{\partial y}\eta +\frac{\partial \Phi }{\partial z}\zeta +\frac{\partial \Phi }{\partial t}\tau +\Phi (\xi ,\eta ,\zeta ,\tau ). \tag {*}

Using the Taylor formula (*), prove that when the origin is moved to the point (ξ,η,ζ)(\xi ,\eta ,\zeta ) the equation of the surface Φ(x,y,z,1)=0\Phi (x,y,z,1) = 0 becomes:

f(x,y,z)+∂Φ∂ξx+∂Φ∂ηy+∂Φ∂ζz+Φ(ξ,η,ζ,1)=0. f(x,y,z)+\frac{\partial \Phi }{\partial \xi }x+\frac{\partial \Phi }{\partial \eta }y+\frac{\partial \Phi }{\partial \zeta }z+\Phi (\xi ,\eta ,\zeta ,1) = 0.
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Problem 578

If the determinant Δ3=∣ADEDBFEFC∣\Delta_{3} = \begin{vmatrix} A & D & E \\ D & B & F \\ E & F & C \end{vmatrix} is nonzero, then it is possible to find ξ\xi, η\eta, and ζ\zeta for which ∂Φ∂ξ=0\dfrac {\partial \Phi }{\partial \xi } = 0, ∂Φ∂η=0\dfrac {\partial \Phi }{\partial \eta } = 0, ∂Φ∂ζ=0\dfrac {\partial \Phi }{\partial \zeta } = 0. Prove that when the origin is moved to the point (ξ,η,ζ)(\xi ,\eta ,\zeta ) the equation of the surface Φ(x,y,z,1)=0\Phi (x,y,z,1) = 0 becomes:

f(x,y,z)+12∂Φ∂t∣t=1=0. f(x,y,z)+\frac{1}{2}\left.\frac{\partial \Phi }{\partial t}\right|_{t=1} = 0.

Here ∂Φ∂t∣t=1\left.\dfrac {\partial \Phi }{\partial t}\right|_{t=1} is the partial derivative taken at t=1t = 1. The indicated shift of origin is the transformation to the center.

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Problem 579

If (x,y,z)(x,y,z) is the midpoint of a chord of the surface Φ(x,y,z,1)=0\Phi (x,y,z,1) = 0 (the notation Φ\Phi and ff is the same as in problem 577), and (x+lσ,y+mσ,z+nσ)(x+l\sigma ,y+m\sigma ,z+n\sigma ) and (x−lσ,y−mσ,z−nσ)(x-l\sigma ,y-m\sigma ,z-n\sigma ) are its endpoints, then the equality

l∂Φ∂x+m∂Φ∂y+n∂Φ∂z=0 l\frac{\partial \Phi }{\partial x}+m\frac{\partial \Phi }{\partial y}+n\frac{\partial \Phi }{\partial z} = 0

holds. Prove this.

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Problem 580

Prove that the midpoints of the chords of the surface Φ(x,y,z,1)=0\Phi (x,y,z,1) = 0 (the notation is the same as in problem 577) parallel to the vector P→(l,m,n)\overrightarrow {P}(l,m,n) lie on the plane

l∂Φ∂x+m∂Φ∂y+n∂Φ∂z=0. l\frac{\partial \Phi }{\partial x}+m\frac{\partial \Phi }{\partial y}+n\frac{\partial \Phi }{\partial z} = 0.

(The diametral plane conjugate to the direction of the vector P→\overrightarrow {P}.)

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Problem 581

Prove that for the surface f(x,y,z)∓k=0f(x,y,z) \mp k = 0 (the notation ff is the same as in problem 577) the equation of the diametral plane conjugate to the direction of the vector P→(l,m,n)\overrightarrow {P}(l,m,n) can be written in either of the two forms:

l∂f∂x+m∂f∂y+n∂f∂z=0 l\frac{\partial f}{\partial x}+m\frac{\partial f}{\partial y}+n\frac{\partial f}{\partial z} = 0

and

∂f(l,m,n)∂lx+∂f(l,m,n)∂my+∂f(l,m,n)∂nz=0. \frac{\partial f(l,m,n)}{\partial l}x+\frac{\partial f(l,m,n)}{\partial m}y+\frac{\partial f(l,m,n)}{\partial n}z = 0.
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Problem 582

Prove that for the surface Φ(x,y,z,1)=0\Phi (x,y,z,1) = 0 (the notation is the same as in problem 577) the equation of the diametral plane conjugate to the direction of the vector P→(l,m,n)\overrightarrow {P}(l,m,n) can be written in the form:

∂f∂lx+∂f∂my+∂f∂nz+∂Φ∂t∣t=0=0. \frac{\partial f}{\partial l}x+\frac{\partial f}{\partial m}y+\frac{\partial f}{\partial n}z+\left.\frac{\partial \Phi }{\partial t}\right|_{t=0} = 0.

Here ∂f∂l\dfrac {\partial f}{\partial l}, ∂f∂m\dfrac {\partial f}{\partial m}, and ∂f∂n\dfrac {\partial f}{\partial n} are the partial derivatives of f(l,m,n)f(l,m,n), and ∂Φ∂t∣t=0\left.\dfrac {\partial \Phi }{\partial t}\right|_{t=0} is the value of the quantity ∂Φ(l,m,n,t)∂t\dfrac {\partial \Phi (l,m,n,t)}{\partial t} at t=0t = 0.

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Problem 583

Find the diametral plane of the surface x2+2y2−z2−2xy−2yz+2xz−4x−1=0x^{2}+2y^{2}-z^{2}-2xy-2yz+2xz-4x-1 = 0 conjugate to the direction of the vector P→(1,−1,0)\overrightarrow {P}(1,-1,0).

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Problem 584

Find the diametral plane of the surface x2+2y2−z2−2xy−2yz+2xz−4x−1=0x^{2}+2y^{2}-z^{2}-2xy-2yz+2xz-4x-1 = 0 parallel to the plane x+y+z=0x+y+z = 0.

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Problem 585

For the same surface find the diametral plane passing through the points (0,0,0)(0,0,0) and (1,1,0)(1,1,0).

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Problem 586

Find the diametral plane of the surface x2+z2−2x−1=0x^{2}+z^{2}-2x-1 = 0 passing through the point (2,1,0)(2,1,0), as well as the direction conjugate to it.

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Problem 587

Find the diametral plane of the surface 4x2+y2+z2+4xy−4xz−2yz+x−y−1=04x^{2}+y^{2}+z^{2}+4xy-4xz-2yz+x-y-1 = 0 passing through the origin.

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Problem 588

Find the equations of the diameter of the surface 4x2+6y2+4z2+4xz+8y−4z+3=04x^{2}+6y^{2}+4z^{2}+4xz+8y-4z+3 = 0 perpendicular to the plane xOzxOz.

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Problem 589

The plane x=0x = 0 is a diametral plane of the surface xy=zxy = z. Find the chords to which it is conjugate.

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Problem 590

Find the diametral plane common to the surfaces x2+y+z=0x^{2}+y+z = 0 and x2+y2−2x−2y−2z=0x^{2}+y^{2}-2x-2y-2z = 0.

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Problem 591

Find the equation of the diameter of the surface x2+2y2−z2−2xy−2yz+2xz−4x−1=0x^{2}+2y^{2}-z^{2}-2xy-2yz+2xz-4x-1 = 0 corresponding to the plane x+y+z−6=0x+y+z-6 = 0.

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Problem 592

Find the locus of the centers of the sections of the surface x2+2y2+2z2−2xy−2yz+2x−2z−1=0x^{2}+2y^{2}+2z^{2}-2xy-2yz+2x-2z-1 = 0 by planes parallel to the plane x−y+z=0x-y+z = 0.

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Problem 593

Given the diameter

{y=z,x−1=0 \begin{cases} y = z, \\ x-1 = 0 \end{cases}

of the surface x2+y2+z2−2yz−2x−y+1=0x^{2}+y^{2}+z^{2}-2yz-2x-y+1 = 0, find the equations of the planes corresponding to it.

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