Se da la ecuación de superficie de 2 grado:
− 3 p + 3 q + x ( p − q ) = 0 - 3 p + 3 q + x \left(p - q\right) = 0 − 3 p + 3 q + x ( p − q ) = 0 Esta ecuación tiene la forma:
a 11 x 2 + 2 a 12 q x + 2 a 13 p x + 2 a 14 x + a 22 q 2 + 2 a 23 p q + 2 a 24 q + a 33 p 2 + 2 a 34 p + a 44 = 0 a_{11} x^{2} + 2 a_{12} q x + 2 a_{13} p x + 2 a_{14} x + a_{22} q^{2} + 2 a_{23} p q + 2 a_{24} q + a_{33} p^{2} + 2 a_{34} p + a_{44} = 0 a 11 x 2 + 2 a 12 q x + 2 a 13 p x + 2 a 14 x + a 22 q 2 + 2 a 23 pq + 2 a 24 q + a 33 p 2 + 2 a 34 p + a 44 = 0 donde
a 11 = 0 a_{11} = 0 a 11 = 0 a 12 = − 1 2 a_{12} = - \frac{1}{2} a 12 = − 2 1 a 13 = 1 2 a_{13} = \frac{1}{2} a 13 = 2 1 a 14 = 0 a_{14} = 0 a 14 = 0 a 22 = 0 a_{22} = 0 a 22 = 0 a 23 = 0 a_{23} = 0 a 23 = 0 a 24 = 3 2 a_{24} = \frac{3}{2} a 24 = 2 3 a 33 = 0 a_{33} = 0 a 33 = 0 a 34 = − 3 2 a_{34} = - \frac{3}{2} a 34 = − 2 3 a 44 = 0 a_{44} = 0 a 44 = 0 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 = 0 I_{1} = 0 I 1 = 0 | 0 -1/2| |0 0| | 0 1/2|
I2 = | | + | | + | |
|-1/2 0 | |0 0| |1/2 0 | I 3 = ∣ 0 − 1 2 1 2 − 1 2 0 0 1 2 0 0 ∣ I_{3} = \left|\begin{matrix}0 & - \frac{1}{2} & \frac{1}{2}\\- \frac{1}{2} & 0 & 0\\\frac{1}{2} & 0 & 0\end{matrix}\right| I 3 = 0 − 2 1 2 1 − 2 1 0 0 2 1 0 0 I 4 = ∣ 0 − 1 2 1 2 0 − 1 2 0 0 3 2 1 2 0 0 − 3 2 0 3 2 − 3 2 0 ∣ I_{4} = \left|\begin{matrix}0 & - \frac{1}{2} & \frac{1}{2} & 0\\- \frac{1}{2} & 0 & 0 & \frac{3}{2}\\\frac{1}{2} & 0 & 0 & - \frac{3}{2}\\0 & \frac{3}{2} & - \frac{3}{2} & 0\end{matrix}\right| I 4 = 0 − 2 1 2 1 0 − 2 1 0 0 2 3 2 1 0 0 − 2 3 0 2 3 − 2 3 0 I ( λ ) = ∣ − λ − 1 2 1 2 − 1 2 − λ 0 1 2 0 − λ ∣ I{\left(\lambda \right)} = \left|\begin{matrix}- \lambda & - \frac{1}{2} & \frac{1}{2}\\- \frac{1}{2} & - \lambda & 0\\\frac{1}{2} & 0 & - \lambda\end{matrix}\right| I ( λ ) = − λ − 2 1 2 1 − 2 1 − λ 0 2 1 0 − λ |0 0| | 0 3/2| | 0 -3/2|
K2 = | | + | | + | |
|0 0| |3/2 0 | |-3/2 0 | | 0 -1/2 0 | | 0 0 3/2 | | 0 1/2 0 |
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K3 = |-1/2 0 3/2| + | 0 0 -3/2| + |1/2 0 -3/2|
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| 0 3/2 0 | |3/2 -3/2 0 | | 0 -3/2 0 | I 1 = 0 I_{1} = 0 I 1 = 0 I 2 = − 1 2 I_{2} = - \frac{1}{2} I 2 = − 2 1 I 3 = 0 I_{3} = 0 I 3 = 0 I 4 = 0 I_{4} = 0 I 4 = 0 I ( λ ) = − λ 3 + λ 2 I{\left(\lambda \right)} = - \lambda^{3} + \frac{\lambda}{2} I ( λ ) = − λ 3 + 2 λ K 2 = − 9 2 K_{2} = - \frac{9}{2} K 2 = − 2 9 K 3 = 0 K_{3} = 0 K 3 = 0 Como
I 3 = 0 ∧ I 4 = 0 ∧ I 2 ≠ 0 I_{3} = 0 \wedge I_{4} = 0 \wedge I_{2} \neq 0 I 3 = 0 ∧ I 4 = 0 ∧ I 2 = 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 − λ 2 = 0 \lambda^{3} - \frac{\lambda}{2} = 0 λ 3 − 2 λ = 0 λ 1 = − 2 2 \lambda_{1} = - \frac{\sqrt{2}}{2} λ 1 = − 2 2 λ 2 = 2 2 \lambda_{2} = \frac{\sqrt{2}}{2} λ 2 = 2 2 λ 3 = 0 \lambda_{3} = 0 λ 3 = 0 entonces la forma canónica de la ecuación será
( q ~ 2 λ 2 + x ~ 2 λ 1 ) + K 3 I 2 = 0 \left(\tilde q^{2} \lambda_{2} + \tilde x^{2} \lambda_{1}\right) + \frac{K_{3}}{I_{2}} = 0 ( q ~ 2 λ 2 + x ~ 2 λ 1 ) + I 2 K 3 = 0 2 q ~ 2 2 − 2 x ~ 2 2 = 0 \frac{\sqrt{2} \tilde q^{2}}{2} - \frac{\sqrt{2} \tilde x^{2}}{2} = 0 2 2 q ~ 2 − 2 2 x ~ 2 = 0 − q ~ 2 ( 2 4 ) 2 + x ~ 2 ( 2 4 ) 2 = 0 - \frac{\tilde q^{2}}{\left(\sqrt[4]{2}\right)^{2}} + \frac{\tilde x^{2}}{\left(\sqrt[4]{2}\right)^{2}} = 0 − ( 4 2 ) 2 q ~ 2 + ( 4 2 ) 2 x ~ 2 = 0 es la ecuación para el tipo dos planos intersectantes
- está reducida a la forma canónica