Se da la ecuación de superficie de 2 grado:
3 x 2 − 12 x + 4 y 2 + 8 y − 24 z + 136 = 0 3 x^{2} - 12 x + 4 y^{2} + 8 y - 24 z + 136 = 0 3 x 2 − 12 x + 4 y 2 + 8 y − 24 z + 136 = 0 Esta ecuación tiene la forma:
a 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 a_{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 a 11 x 2 + 2 a 12 x y + 2 a 13 x z + 2 a 14 x + a 22 y 2 + 2 a 23 yz + 2 a 24 y + a 33 z 2 + 2 a 34 z + a 44 = 0 donde
a 11 = 3 a_{11} = 3 a 11 = 3 a 12 = 0 a_{12} = 0 a 12 = 0 a 13 = 0 a_{13} = 0 a 13 = 0 a 14 = − 6 a_{14} = -6 a 14 = − 6 a 22 = 4 a_{22} = 4 a 22 = 4 a 23 = 0 a_{23} = 0 a 23 = 0 a 24 = 4 a_{24} = 4 a 24 = 4 a 33 = 0 a_{33} = 0 a 33 = 0 a 34 = − 12 a_{34} = -12 a 34 = − 12 a 44 = 136 a_{44} = 136 a 44 = 136 Las invariantes de esta ecuación al transformar las coordenadas son los determinantes:
I 1 = a 11 + a 22 + a 33 I_{1} = a_{11} + a_{22} + a_{33} I 1 = a 11 + a 22 + a 33 |a11 a12| |a22 a23| |a11 a13|
I2 = | | + | | + | |
|a12 a22| |a23 a33| |a13 a33| I 3 = ∣ a 11 a 12 a 13 a 12 a 22 a 23 a 13 a 23 a 33 ∣ I_{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| I 3 = a 11 a 12 a 13 a 12 a 22 a 23 a 13 a 23 a 33 I 4 = ∣ 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 ∣ I_{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 4 = 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 I ( λ ) = ∣ a 11 − λ a 12 a 13 a 12 a 22 − λ a 23 a 13 a 23 a 33 − λ ∣ I{\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| I ( λ ) = a 11 − λ a 12 a 13 a 12 a 22 − λ a 23 a 13 a 23 a 33 − λ |a11 a14| |a22 a24| |a33 a34|
K2 = | | + | | + | |
|a14 a44| |a24 a44| |a34 a44| |a11 a12 a14| |a22 a23 a24| |a11 a13 a14|
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K3 = |a12 a22 a24| + |a23 a33 a34| + |a13 a33 a34|
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|a14 a24 a44| |a24 a34 a44| |a14 a34 a44| sustituimos coeficientes
I 1 = 7 I_{1} = 7 I 1 = 7 |3 0| |4 0| |3 0|
I2 = | | + | | + | |
|0 4| |0 0| |0 0| I 3 = ∣ 3 0 0 0 4 0 0 0 0 ∣ I_{3} = \left|\begin{matrix}3 & 0 & 0\\0 & 4 & 0\\0 & 0 & 0\end{matrix}\right| I 3 = 3 0 0 0 4 0 0 0 0 I 4 = ∣ 3 0 0 − 6 0 4 0 4 0 0 0 − 12 − 6 4 − 12 136 ∣ I_{4} = \left|\begin{matrix}3 & 0 & 0 & -6\\0 & 4 & 0 & 4\\0 & 0 & 0 & -12\\-6 & 4 & -12 & 136\end{matrix}\right| I 4 = 3 0 0 − 6 0 4 0 4 0 0 0 − 12 − 6 4 − 12 136 I ( λ ) = ∣ 3 − λ 0 0 0 4 − λ 0 0 0 − λ ∣ I{\left(\lambda \right)} = \left|\begin{matrix}3 - \lambda & 0 & 0\\0 & 4 - \lambda & 0\\0 & 0 & - \lambda\end{matrix}\right| I ( λ ) = 3 − λ 0 0 0 4 − λ 0 0 0 − λ |3 -6 | |4 4 | | 0 -12|
K2 = | | + | | + | |
|-6 136| |4 136| |-12 136| |3 0 -6 | |4 0 4 | |3 0 -6 |
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K3 = |0 4 4 | + |0 0 -12| + |0 0 -12|
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|-6 4 136| |4 -12 136| |-6 -12 136| I 1 = 7 I_{1} = 7 I 1 = 7 I 2 = 12 I_{2} = 12 I 2 = 12 I 3 = 0 I_{3} = 0 I 3 = 0 I 4 = − 1728 I_{4} = -1728 I 4 = − 1728 I ( λ ) = − λ 3 + 7 λ 2 − 12 λ I{\left(\lambda \right)} = - \lambda^{3} + 7 \lambda^{2} - 12 \lambda I ( λ ) = − λ 3 + 7 λ 2 − 12 λ K 2 = 756 K_{2} = 756 K 2 = 756 K 3 = 432 K_{3} = 432 K 3 = 432 Como
I 3 = 0 ∧ I 2 ≠ 0 ∧ I 4 ≠ 0 I_{3} = 0 \wedge I_{2} \neq 0 \wedge I_{4} \neq 0 I 3 = 0 ∧ I 2 = 0 ∧ I 4 = 0 entonces por razón de tipos de rectas:
hay que
Formulamos la ecuación característica para nuestra superficie:
− I 1 λ 2 + I 2 λ − I 3 + λ 3 = 0 - I_{1} \lambda^{2} + I_{2} \lambda - I_{3} + \lambda^{3} = 0 − I 1 λ 2 + I 2 λ − I 3 + λ 3 = 0 o
λ 3 − 7 λ 2 + 12 λ = 0 \lambda^{3} - 7 \lambda^{2} + 12 \lambda = 0 λ 3 − 7 λ 2 + 12 λ = 0 λ 1 = 4 \lambda_{1} = 4 λ 1 = 4 λ 2 = 3 \lambda_{2} = 3 λ 2 = 3 λ 3 = 0 \lambda_{3} = 0 λ 3 = 0 entonces la forma canónica de la ecuación será
z ~ 2 ( − 1 ) I 4 I 2 + ( x ~ 2 λ 1 + y ~ 2 λ 2 ) = 0 \tilde z 2 \sqrt{\frac{\left(-1\right) I_{4}}{I_{2}}} + \left(\tilde x^{2} \lambda_{1} + \tilde y^{2} \lambda_{2}\right) = 0 z ~ 2 I 2 ( − 1 ) I 4 + ( x ~ 2 λ 1 + y ~ 2 λ 2 ) = 0 y
− z ~ 2 ( − 1 ) I 4 I 2 + ( x ~ 2 λ 1 + y ~ 2 λ 2 ) = 0 - \tilde z 2 \sqrt{\frac{\left(-1\right) I_{4}}{I_{2}}} + \left(\tilde x^{2} \lambda_{1} + \tilde y^{2} \lambda_{2}\right) = 0 − z ~ 2 I 2 ( − 1 ) I 4 + ( x ~ 2 λ 1 + y ~ 2 λ 2 ) = 0 4 x ~ 2 + 3 y ~ 2 + 24 z ~ = 0 4 \tilde x^{2} + 3 \tilde y^{2} + 24 \tilde z = 0 4 x ~ 2 + 3 y ~ 2 + 24 z ~ = 0 y
4 x ~ 2 + 3 y ~ 2 − 24 z ~ = 0 4 \tilde x^{2} + 3 \tilde y^{2} - 24 \tilde z = 0 4 x ~ 2 + 3 y ~ 2 − 24 z ~ = 0 2 z ~ + ( x ~ 2 3 + y ~ 2 4 ) = 0 2 \tilde z + \left(\frac{\tilde x^{2}}{3} + \frac{\tilde y^{2}}{4}\right) = 0 2 z ~ + ( 3 x ~ 2 + 4 y ~ 2 ) = 0 y
− 2 z ~ + ( x ~ 2 3 + y ~ 2 4 ) = 0 - 2 \tilde z + \left(\frac{\tilde x^{2}}{3} + \frac{\tilde y^{2}}{4}\right) = 0 − 2 z ~ + ( 3 x ~ 2 + 4 y ~ 2 ) = 0 es la ecuación para el tipo paraboloide elíptico
- está reducida a la forma canónica