Se da la ecuación de superficie de 2 grado:
4 x 2 + y 2 − 4 y + 4 z 2 − 24 z + 36 = 0 4 x^{2} + y^{2} - 4 y + 4 z^{2} - 24 z + 36 = 0 4 x 2 + y 2 − 4 y + 4 z 2 − 24 z + 36 = 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 = 4 a_{11} = 4 a 11 = 4 a 12 = 0 a_{12} = 0 a 12 = 0 a 13 = 0 a_{13} = 0 a 13 = 0 a 14 = 0 a_{14} = 0 a 14 = 0 a 22 = 1 a_{22} = 1 a 22 = 1 a 23 = 0 a_{23} = 0 a 23 = 0 a 24 = − 2 a_{24} = -2 a 24 = − 2 a 33 = 4 a_{33} = 4 a 33 = 4 a 34 = − 12 a_{34} = -12 a 34 = − 12 a 44 = 36 a_{44} = 36 a 44 = 36 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|
| | | | | |
K3 = |a12 a22 a24| + |a23 a33 a34| + |a13 a33 a34|
| | | | | |
|a14 a24 a44| |a24 a34 a44| |a14 a34 a44| sustituimos coeficientes
I 1 = 9 I_{1} = 9 I 1 = 9 |4 0| |1 0| |4 0|
I2 = | | + | | + | |
|0 1| |0 4| |0 4| I 3 = ∣ 4 0 0 0 1 0 0 0 4 ∣ I_{3} = \left|\begin{matrix}4 & 0 & 0\\0 & 1 & 0\\0 & 0 & 4\end{matrix}\right| I 3 = 4 0 0 0 1 0 0 0 4 I 4 = ∣ 4 0 0 0 0 1 0 − 2 0 0 4 − 12 0 − 2 − 12 36 ∣ I_{4} = \left|\begin{matrix}4 & 0 & 0 & 0\\0 & 1 & 0 & -2\\0 & 0 & 4 & -12\\0 & -2 & -12 & 36\end{matrix}\right| I 4 = 4 0 0 0 0 1 0 − 2 0 0 4 − 12 0 − 2 − 12 36 I ( λ ) = ∣ 4 − λ 0 0 0 1 − λ 0 0 0 4 − λ ∣ I{\left(\lambda \right)} = \left|\begin{matrix}4 - \lambda & 0 & 0\\0 & 1 - \lambda & 0\\0 & 0 & 4 - \lambda\end{matrix}\right| I ( λ ) = 4 − λ 0 0 0 1 − λ 0 0 0 4 − λ |4 0 | |1 -2| | 4 -12|
K2 = | | + | | + | |
|0 36| |-2 36| |-12 36 | |4 0 0 | |1 0 -2 | |4 0 0 |
| | | | | |
K3 = |0 1 -2| + |0 4 -12| + |0 4 -12|
| | | | | |
|0 -2 36| |-2 -12 36 | |0 -12 36 | I 1 = 9 I_{1} = 9 I 1 = 9 I 2 = 24 I_{2} = 24 I 2 = 24 I 3 = 16 I_{3} = 16 I 3 = 16 I 4 = − 64 I_{4} = -64 I 4 = − 64 I ( λ ) = − λ 3 + 9 λ 2 − 24 λ + 16 I{\left(\lambda \right)} = - \lambda^{3} + 9 \lambda^{2} - 24 \lambda + 16 I ( λ ) = − λ 3 + 9 λ 2 − 24 λ + 16 K 2 = 176 K_{2} = 176 K 2 = 176 K 3 = 112 K_{3} = 112 K 3 = 112 Como
I3 != 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 − 9 λ 2 + 24 λ − 16 = 0 \lambda^{3} - 9 \lambda^{2} + 24 \lambda - 16 = 0 λ 3 − 9 λ 2 + 24 λ − 16 = 0 λ 1 = 1 \lambda_{1} = 1 λ 1 = 1 λ 2 = 4 \lambda_{2} = 4 λ 2 = 4 λ 3 = 4 \lambda_{3} = 4 λ 3 = 4 entonces la forma canónica de la ecuación será
( z ~ 2 λ 3 + ( x ~ 2 λ 1 + y ~ 2 λ 2 ) ) + I 4 I 3 = 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 ( z ~ 2 λ 3 + ( x ~ 2 λ 1 + y ~ 2 λ 2 ) ) + I 3 I 4 = 0 x ~ 2 + 4 y ~ 2 + 4 z ~ 2 − 4 = 0 \tilde x^{2} + 4 \tilde y^{2} + 4 \tilde z^{2} - 4 = 0 x ~ 2 + 4 y ~ 2 + 4 z ~ 2 − 4 = 0 2 2 2
\tilde x \tilde y \tilde z
--------- + --------- + --------- = 1
2 2 2
/ 1\ / 1 \ / 1 \
\2 / |-----| |-----|
\2*1/2/ \2*1/2/ es la ecuación para el tipo elipsoide
- está reducida a la forma canónica