Given equation of the surface of 2-order:
− 7 x y + 2 z 2 = 0 - 7 x y + 2 z^{2} = 0 − 7 x y + 2 z 2 = 0 This equation looks like:
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 where
a 11 = 0 a_{11} = 0 a 11 = 0 a 12 = − 7 2 a_{12} = - \frac{7}{2} a 12 = − 2 7 a 13 = 0 a_{13} = 0 a 13 = 0 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 = 0 a_{24} = 0 a 24 = 0 a 33 = 2 a_{33} = 2 a 33 = 2 a 34 = 0 a_{34} = 0 a 34 = 0 a 44 = 0 a_{44} = 0 a 44 = 0 The invariants of the equation when converting coordinates are determinants:
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| substitute coefficients
I 1 = 2 I_{1} = 2 I 1 = 2 | 0 -7/2| |0 0| |0 0|
I2 = | | + | | + | |
|-7/2 0 | |0 2| |0 2| I 3 = ∣ 0 − 7 2 0 − 7 2 0 0 0 0 2 ∣ I_{3} = \left|\begin{matrix}0 & - \frac{7}{2} & 0\\- \frac{7}{2} & 0 & 0\\0 & 0 & 2\end{matrix}\right| I 3 = 0 − 2 7 0 − 2 7 0 0 0 0 2 I 4 = ∣ 0 − 7 2 0 0 − 7 2 0 0 0 0 0 2 0 0 0 0 0 ∣ I_{4} = \left|\begin{matrix}0 & - \frac{7}{2} & 0 & 0\\- \frac{7}{2} & 0 & 0 & 0\\0 & 0 & 2 & 0\\0 & 0 & 0 & 0\end{matrix}\right| I 4 = 0 − 2 7 0 0 − 2 7 0 0 0 0 0 2 0 0 0 0 0 I ( λ ) = ∣ − λ − 7 2 0 − 7 2 − λ 0 0 0 2 − λ ∣ I{\left(\lambda \right)} = \left|\begin{matrix}- \lambda & - \frac{7}{2} & 0\\- \frac{7}{2} & - \lambda & 0\\0 & 0 & 2 - \lambda\end{matrix}\right| I ( λ ) = − λ − 2 7 0 − 2 7 − λ 0 0 0 2 − λ |0 0| |0 0| |2 0|
K2 = | | + | | + | |
|0 0| |0 0| |0 0| | 0 -7/2 0| |0 0 0| |0 0 0|
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K3 = |-7/2 0 0| + |0 2 0| + |0 2 0|
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| 0 0 0| |0 0 0| |0 0 0| I 1 = 2 I_{1} = 2 I 1 = 2 I 2 = − 49 4 I_{2} = - \frac{49}{4} I 2 = − 4 49 I 3 = − 49 2 I_{3} = - \frac{49}{2} I 3 = − 2 49 I 4 = 0 I_{4} = 0 I 4 = 0 I ( λ ) = − λ 3 + 2 λ 2 + 49 λ 4 − 49 2 I{\left(\lambda \right)} = - \lambda^{3} + 2 \lambda^{2} + \frac{49 \lambda}{4} - \frac{49}{2} I ( λ ) = − λ 3 + 2 λ 2 + 4 49 λ − 2 49 K 2 = 0 K_{2} = 0 K 2 = 0 K 3 = 0 K_{3} = 0 K 3 = 0 Because
I3 != 0 then by type of surface:
you need to
Make the characteristic equation for the surface:
− 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 or
λ 3 − 2 λ 2 − 49 λ 4 + 49 2 = 0 \lambda^{3} - 2 \lambda^{2} - \frac{49 \lambda}{4} + \frac{49}{2} = 0 λ 3 − 2 λ 2 − 4 49 λ + 2 49 = 0 λ 1 = 2 \lambda_{1} = 2 λ 1 = 2 λ 2 = 7 2 \lambda_{2} = \frac{7}{2} λ 2 = 2 7 λ 3 = − 7 2 \lambda_{3} = - \frac{7}{2} λ 3 = − 2 7 then the canonical form of the equation will be
( 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 2 x ~ 2 + 7 y ~ 2 2 − 7 z ~ 2 2 = 0 2 \tilde x^{2} + \frac{7 \tilde y^{2}}{2} - \frac{7 \tilde z^{2}}{2} = 0 2 x ~ 2 + 2 7 y ~ 2 − 2 7 z ~ 2 = 0 − z ~ 2 ( 14 7 ) 2 + ( x ~ 2 ( 2 2 ) 2 + y ~ 2 ( 14 7 ) 2 ) = 0 - \frac{\tilde z^{2}}{\left(\frac{\sqrt{14}}{7}\right)^{2}} + \left(\frac{\tilde x^{2}}{\left(\frac{\sqrt{2}}{2}\right)^{2}} + \frac{\tilde y^{2}}{\left(\frac{\sqrt{14}}{7}\right)^{2}}\right) = 0 − ( 7 14 ) 2 z ~ 2 + ( 2 2 ) 2 x ~ 2 + ( 7 14 ) 2 y ~ 2 = 0 this equation is fora type cone
- reduced to canonical form