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6x^2-y^2+3z^2-12=0 forma canónica

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y: [, ]
z: [, ]

Calidad:

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Solución

Ha introducido [src]
       2      2      2    
-12 - y  + 3*z  + 6*x  = 0
6x2y2+3z212=06 x^{2} - y^{2} + 3 z^{2} - 12 = 0
6*x^2 - y^2 + 3*z^2 - 12 = 0
Método de invariantes
Se da la ecuación de superficie de 2 grado:
6x2y2+3z212=06 x^{2} - y^{2} + 3 z^{2} - 12 = 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=6a_{11} = 6
a12=0a_{12} = 0
a13=0a_{13} = 0
a14=0a_{14} = 0
a22=1a_{22} = -1
a23=0a_{23} = 0
a24=0a_{24} = 0
a33=3a_{33} = 3
a34=0a_{34} = 0
a44=12a_{44} = -12
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=8I_{1} = 8
     |6  0 |   |-1  0|   |6  0|
I2 = |     | + |     | + |    |
     |0  -1|   |0   3|   |0  3|

I3=600010003I_{3} = \left|\begin{matrix}6 & 0 & 0\\0 & -1 & 0\\0 & 0 & 3\end{matrix}\right|
I4=60000100003000012I_{4} = \left|\begin{matrix}6 & 0 & 0 & 0\\0 & -1 & 0 & 0\\0 & 0 & 3 & 0\\0 & 0 & 0 & -12\end{matrix}\right|
I(λ)=6λ000λ10003λI{\left(\lambda \right)} = \left|\begin{matrix}6 - \lambda & 0 & 0\\0 & - \lambda - 1 & 0\\0 & 0 & 3 - \lambda\end{matrix}\right|
     |6   0 |   |-1   0 |   |3   0 |
K2 = |      | + |       | + |      |
     |0  -12|   |0   -12|   |0  -12|

     |6  0    0 |   |-1  0   0 |   |6  0   0 |
     |          |   |          |   |         |
K3 = |0  -1   0 | + |0   3   0 | + |0  3   0 |
     |          |   |          |   |         |
     |0  0   -12|   |0   0  -12|   |0  0  -12|

I1=8I_{1} = 8
I2=9I_{2} = 9
I3=18I_{3} = -18
I4=216I_{4} = 216
I(λ)=λ3+8λ29λ18I{\left(\lambda \right)} = - \lambda^{3} + 8 \lambda^{2} - 9 \lambda - 18
K2=96K_{2} = -96
K3=108K_{3} = -108
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
λ38λ2+9λ+18=0\lambda^{3} - 8 \lambda^{2} + 9 \lambda + 18 = 0
λ1=6\lambda_{1} = 6
λ2=3\lambda_{2} = 3
λ3=1\lambda_{3} = -1
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
6x~2+3y~2z~212=06 \tilde x^{2} + 3 \tilde y^{2} - \tilde z^{2} - 12 = 0
z~2(1163)2+(x~2(166163)2+y~2(133163)2)=1- \frac{\tilde z^{2}}{\left(\frac{1}{\frac{1}{6} \sqrt{3}}\right)^{2}} + \left(\frac{\tilde x^{2}}{\left(\frac{\frac{1}{6} \sqrt{6}}{\frac{1}{6} \sqrt{3}}\right)^{2}} + \frac{\tilde y^{2}}{\left(\frac{\frac{1}{3} \sqrt{3}}{\frac{1}{6} \sqrt{3}}\right)^{2}}\right) = 1
es la ecuación para el tipo hiperboloide unilateral
- está reducida a la forma canónica