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x^2-2*x*y+2*x*z+y*z+z^2=0 forma canónica

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x: [, ]
y: [, ]
z: [, ]

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Solución

Ha introducido [src]
 2    2                          
x  + z  + y*z - 2*x*y + 2*x*z = 0
x22xy+2xz+yz+z2=0x^{2} - 2 x y + 2 x z + y z + z^{2} = 0
x^2 - 2*x*y + 2*x*z + y*z + z^2 = 0
Método de invariantes
Se da la ecuación de superficie de 2 grado:
x22xy+2xz+yz+z2=0x^{2} - 2 x y + 2 x z + y z + z^{2} = 0
Esta ecuación tiene la forma:
a11x2+2a12xy+2a13xz+2a14x+a22y2+2a23yz+2a24y+a33z2+2a34z+a44=0a_{11} x^{2} + 2 a_{12} x y + 2 a_{13} x z + 2 a_{14} x + a_{22} y^{2} + 2 a_{23} y z + 2 a_{24} y + a_{33} z^{2} + 2 a_{34} z + a_{44} = 0
donde
a11=1a_{11} = 1
a12=1a_{12} = -1
a13=1a_{13} = 1
a14=0a_{14} = 0
a22=0a_{22} = 0
a23=12a_{23} = \frac{1}{2}
a24=0a_{24} = 0
a33=1a_{33} = 1
a34=0a_{34} = 0
a44=0a_{44} = 0
Las invariantes de esta ecuación al transformar las coordenadas son los determinantes:
I1=a11+a22+a33I_{1} = a_{11} + a_{22} + a_{33}
     |a11  a12|   |a22  a23|   |a11  a13|
I2 = |        | + |        | + |        |
     |a12  a22|   |a23  a33|   |a13  a33|

I3=a11a12a13a12a22a23a13a23a33I_{3} = \left|\begin{matrix}a_{11} & a_{12} & a_{13}\\a_{12} & a_{22} & a_{23}\\a_{13} & a_{23} & a_{33}\end{matrix}\right|
I4=a11a12a13a14a12a22a23a24a13a23a33a34a14a24a34a44I_{4} = \left|\begin{matrix}a_{11} & a_{12} & a_{13} & a_{14}\\a_{12} & a_{22} & a_{23} & a_{24}\\a_{13} & a_{23} & a_{33} & a_{34}\\a_{14} & a_{24} & a_{34} & a_{44}\end{matrix}\right|
I(λ)=a11λa12a13a12a22λa23a13a23a33λI{\left(\lambda \right)} = \left|\begin{matrix}a_{11} - \lambda & a_{12} & a_{13}\\a_{12} & a_{22} - \lambda & a_{23}\\a_{13} & a_{23} & a_{33} - \lambda\end{matrix}\right|
     |a11  a14|   |a22  a24|   |a33  a34|
K2 = |        | + |        | + |        |
     |a14  a44|   |a24  a44|   |a34  a44|

     |a11  a12  a14|   |a22  a23  a24|   |a11  a13  a14|
     |             |   |             |   |             |
K3 = |a12  a22  a24| + |a23  a33  a34| + |a13  a33  a34|
     |             |   |             |   |             |
     |a14  a24  a44|   |a24  a34  a44|   |a14  a34  a44|

sustituimos coeficientes
I1=2I_{1} = 2
     |1   -1|   | 0   1/2|   |1  1|
I2 = |      | + |        | + |    |
     |-1  0 |   |1/2   1 |   |1  1|

I3=11110121121I_{3} = \left|\begin{matrix}1 & -1 & 1\\-1 & 0 & \frac{1}{2}\\1 & \frac{1}{2} & 1\end{matrix}\right|
I4=111010120112100000I_{4} = \left|\begin{matrix}1 & -1 & 1 & 0\\-1 & 0 & \frac{1}{2} & 0\\1 & \frac{1}{2} & 1 & 0\\0 & 0 & 0 & 0\end{matrix}\right|
I(λ)=1λ111λ121121λI{\left(\lambda \right)} = \left|\begin{matrix}1 - \lambda & -1 & 1\\-1 & - \lambda & \frac{1}{2}\\1 & \frac{1}{2} & 1 - \lambda\end{matrix}\right|
     |1  0|   |0  0|   |1  0|
K2 = |    | + |    | + |    |
     |0  0|   |0  0|   |0  0|

     |1   -1  0|   | 0   1/2  0|   |1  1  0|
     |         |   |           |   |       |
K3 = |-1  0   0| + |1/2   1   0| + |1  1  0|
     |         |   |           |   |       |
     |0   0   0|   | 0    0   0|   |0  0  0|

I1=2I_{1} = 2
I2=54I_{2} = - \frac{5}{4}
I3=94I_{3} = - \frac{9}{4}
I4=0I_{4} = 0
I(λ)=λ3+2λ2+5λ494I{\left(\lambda \right)} = - \lambda^{3} + 2 \lambda^{2} + \frac{5 \lambda}{4} - \frac{9}{4}
K2=0K_{2} = 0
K3=0K_{3} = 0
Como
I3 != 0

entonces por razón de tipos de rectas:
hay que
Formulamos la ecuación característica para nuestra superficie:
I1λ2+I2λI3+λ3=0- I_{1} \lambda^{2} + I_{2} \lambda - I_{3} + \lambda^{3} = 0
o
λ32λ25λ4+94=0\lambda^{3} - 2 \lambda^{2} - \frac{5 \lambda}{4} + \frac{9}{4} = 0
λ1=1\lambda_{1} = 1
λ2=12102\lambda_{2} = \frac{1}{2} - \frac{\sqrt{10}}{2}
λ3=12+102\lambda_{3} = \frac{1}{2} + \frac{\sqrt{10}}{2}
entonces la forma canónica de la ecuación será
(z~2λ3+(x~2λ1+y~2λ2))+I4I3=0\left(\tilde z^{2} \lambda_{3} + \left(\tilde x^{2} \lambda_{1} + \tilde y^{2} \lambda_{2}\right)\right) + \frac{I_{4}}{I_{3}} = 0
x~2+y~2(12102)+z~2(12+102)=0\tilde x^{2} + \tilde y^{2} \left(\frac{1}{2} - \frac{\sqrt{10}}{2}\right) + \tilde z^{2} \left(\frac{1}{2} + \frac{\sqrt{10}}{2}\right) = 0
y~2(112+102)2+(x~212+z~2(112+102)2)=0- \frac{\tilde y^{2}}{\left(\frac{1}{\sqrt{- \frac{1}{2} + \frac{\sqrt{10}}{2}}}\right)^{2}} + \left(\frac{\tilde x^{2}}{1^{2}} + \frac{\tilde z^{2}}{\left(\frac{1}{\sqrt{\frac{1}{2} + \frac{\sqrt{10}}{2}}}\right)^{2}}\right) = 0
es la ecuación para el tipo cono
- está reducida a la forma canónica