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4x^2-3y^2-2xy+z^2+6z+5=0 canonical form

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     2      2      2                  
5 + z  - 3*y  + 4*x  + 6*z - 2*x*y = 0
$$4 x^{2} - 2 x y - 3 y^{2} + z^{2} + 6 z + 5 = 0$$
4*x^2 - 2*x*y - 3*y^2 + z^2 + 6*z + 5 = 0
Invariants method
Given equation of the surface of 2-order:
$$4 x^{2} - 2 x y - 3 y^{2} + z^{2} + 6 z + 5 = 0$$
This equation looks like:
$$a_{11} x^{2} + 2 a_{12} x y + 2 a_{13} x z + 2 a_{14} x + a_{22} y^{2} + 2 a_{23} y z + 2 a_{24} y + a_{33} z^{2} + 2 a_{34} z + a_{44} = 0$$
where
$$a_{11} = 4$$
$$a_{12} = -1$$
$$a_{13} = 0$$
$$a_{14} = 0$$
$$a_{22} = -3$$
$$a_{23} = 0$$
$$a_{24} = 0$$
$$a_{33} = 1$$
$$a_{34} = 3$$
$$a_{44} = 5$$
The invariants of the equation when converting coordinates are determinants:
$$I_{1} = a_{11} + a_{22} + a_{33}$$
     |a11  a12|   |a22  a23|   |a11  a13|
I2 = |        | + |        | + |        |
     |a12  a22|   |a23  a33|   |a13  a33|

$$I_{3} = \left|\begin{matrix}a_{11} & a_{12} & a_{13}\\a_{12} & a_{22} & a_{23}\\a_{13} & a_{23} & a_{33}\end{matrix}\right|$$
$$I_{4} = \left|\begin{matrix}a_{11} & a_{12} & a_{13} & a_{14}\\a_{12} & a_{22} & a_{23} & a_{24}\\a_{13} & a_{23} & a_{33} & a_{34}\\a_{14} & a_{24} & a_{34} & a_{44}\end{matrix}\right|$$
$$I{\left(\lambda \right)} = \left|\begin{matrix}a_{11} - \lambda & a_{12} & a_{13}\\a_{12} & a_{22} - \lambda & a_{23}\\a_{13} & a_{23} & a_{33} - \lambda\end{matrix}\right|$$
     |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|

substitute coefficients
$$I_{1} = 2$$
     |4   -1|   |-3  0|   |4  0|
I2 = |      | + |     | + |    |
     |-1  -3|   |0   1|   |0  1|

$$I_{3} = \left|\begin{matrix}4 & -1 & 0\\-1 & -3 & 0\\0 & 0 & 1\end{matrix}\right|$$
$$I_{4} = \left|\begin{matrix}4 & -1 & 0 & 0\\-1 & -3 & 0 & 0\\0 & 0 & 1 & 3\\0 & 0 & 3 & 5\end{matrix}\right|$$
$$I{\left(\lambda \right)} = \left|\begin{matrix}4 - \lambda & -1 & 0\\-1 & - \lambda - 3 & 0\\0 & 0 & 1 - \lambda\end{matrix}\right|$$
     |4  0|   |-3  0|   |1  3|
K2 = |    | + |     | + |    |
     |0  5|   |0   5|   |3  5|

     |4   -1  0|   |-3  0  0|   |4  0  0|
     |         |   |        |   |       |
K3 = |-1  -3  0| + |0   1  3| + |0  1  3|
     |         |   |        |   |       |
     |0   0   5|   |0   3  5|   |0  3  5|

$$I_{1} = 2$$
$$I_{2} = -12$$
$$I_{3} = -13$$
$$I_{4} = 52$$
$$I{\left(\lambda \right)} = - \lambda^{3} + 2 \lambda^{2} + 12 \lambda - 13$$
$$K_{2} = 1$$
$$K_{3} = -69$$
Because
I3 != 0

then by type of surface:
you need to
Make the characteristic equation for the surface:
$$- I_{1} \lambda^{2} + I_{2} \lambda - I_{3} + \lambda^{3} = 0$$
or
$$\lambda^{3} - 2 \lambda^{2} - 12 \lambda + 13 = 0$$
$$\lambda_{1} = 1$$
$$\lambda_{2} = \frac{1}{2} - \frac{\sqrt{53}}{2}$$
$$\lambda_{3} = \frac{1}{2} + \frac{\sqrt{53}}{2}$$
then the canonical form of the equation will be
$$\left(\tilde z^{2} \lambda_{3} + \left(\tilde x^{2} \lambda_{1} + \tilde y^{2} \lambda_{2}\right)\right) + \frac{I_{4}}{I_{3}} = 0$$
$$\tilde x^{2} + \tilde y^{2} \left(\frac{1}{2} - \frac{\sqrt{53}}{2}\right) + \tilde z^{2} \left(\frac{1}{2} + \frac{\sqrt{53}}{2}\right) - 4 = 0$$
        2                  2                           2             
\tilde x           \tilde z                    \tilde y              
--------- + ------------------------ - -------------------------- = 1
      2                            2                            2    
  / 1\      /          1          \    /           1           \     
  \2 /      |---------------------|    |-----------------------|     
            |     ____________    |    |     ______________    |     
            |    /       ____     |    |    /         ____     |     
            |   /  1   \/ 53      |    |   /    1   \/ 53      |     
            |  /   - + ------ *1/2|    |  /   - - + ------ *1/2|     
            \\/    2     2        /    \\/      2     2        /     

this equation is fora type one-sided hyperboloid
- reduced to canonical form