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(-3)x^2+4xy+(-3)y^2+(-6)x+4y+2=0 canonical form

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             2      2                  
2 - 6*x - 3*x  - 3*y  + 4*y + 4*x*y = 0
$$- 3 x^{2} + 4 x y - 6 x - 3 y^{2} + 4 y + 2 = 0$$
-3*x^2 + 4*x*y - 6*x - 3*y^2 + 4*y + 2 = 0
Detail solution
Given line equation of 2-order:
$$- 3 x^{2} + 4 x y - 6 x - 3 y^{2} + 4 y + 2 = 0$$
This equation looks like:
$$a_{11} x^{2} + 2 a_{12} x y + 2 a_{13} x + a_{22} y^{2} + 2 a_{23} y + a_{33} = 0$$
where
$$a_{11} = -3$$
$$a_{12} = 2$$
$$a_{13} = -3$$
$$a_{22} = -3$$
$$a_{23} = 2$$
$$a_{33} = 2$$
To calculate the determinant
$$\Delta = \left|\begin{matrix}a_{11} & a_{12}\\a_{12} & a_{22}\end{matrix}\right|$$
or, substitute
$$\Delta = \left|\begin{matrix}-3 & 2\\2 & -3\end{matrix}\right|$$
$$\Delta = 5$$
Because
$$\Delta$$
is not equal to 0, then
find the center of the canonical coordinate system. To do it, solve the system of equations
$$a_{11} x_{0} + a_{12} y_{0} + a_{13} = 0$$
$$a_{12} x_{0} + a_{22} y_{0} + a_{23} = 0$$
substitute coefficients
$$- 3 x_{0} + 2 y_{0} - 3 = 0$$
$$2 x_{0} - 3 y_{0} + 2 = 0$$
then
$$x_{0} = -1$$
$$y_{0} = 0$$
Thus, we have the equation in the coordinate system O'x'y'
$$a'_{33} + a_{11} x'^{2} + 2 a_{12} x' y' + a_{22} y'^{2} = 0$$
where
$$a'_{33} = a_{13} x_{0} + a_{23} y_{0} + a_{33}$$
or
$$a'_{33} = - 3 x_{0} + 2 y_{0} + 2$$
$$a'_{33} = 5$$
then equation turns into
$$- 3 x'^{2} + 4 x' y' - 3 y'^{2} + 5 = 0$$
Rotate the resulting coordinate system by an angle φ
$$x' = \tilde x \cos{\left(\phi \right)} - \tilde y \sin{\left(\phi \right)}$$
$$y' = \tilde x \sin{\left(\phi \right)} + \tilde y \cos{\left(\phi \right)}$$
φ - determined from the formula
$$\cot{\left(2 \phi \right)} = \frac{a_{11} - a_{22}}{2 a_{12}}$$
substitute coefficients
$$\cot{\left(2 \phi \right)} = 0$$
then
$$\phi = \frac{\pi}{4}$$
$$\sin{\left(2 \phi \right)} = 1$$
$$\cos{\left(2 \phi \right)} = 0$$
$$\cos{\left(\phi \right)} = \sqrt{\frac{\cos{\left(2 \phi \right)}}{2} + \frac{1}{2}}$$
$$\sin{\left(\phi \right)} = \sqrt{1 - \cos^{2}{\left(\phi \right)}}$$
$$\cos{\left(\phi \right)} = \frac{\sqrt{2}}{2}$$
$$\sin{\left(\phi \right)} = \frac{\sqrt{2}}{2}$$
substitute coefficients
$$x' = \frac{\sqrt{2} \tilde x}{2} - \frac{\sqrt{2} \tilde y}{2}$$
$$y' = \frac{\sqrt{2} \tilde x}{2} + \frac{\sqrt{2} \tilde y}{2}$$
then the equation turns from
$$- 3 x'^{2} + 4 x' y' - 3 y'^{2} + 5 = 0$$
to
$$- 3 \left(\frac{\sqrt{2} \tilde x}{2} - \frac{\sqrt{2} \tilde y}{2}\right)^{2} + 4 \left(\frac{\sqrt{2} \tilde x}{2} - \frac{\sqrt{2} \tilde y}{2}\right) \left(\frac{\sqrt{2} \tilde x}{2} + \frac{\sqrt{2} \tilde y}{2}\right) - 3 \left(\frac{\sqrt{2} \tilde x}{2} + \frac{\sqrt{2} \tilde y}{2}\right)^{2} + 5 = 0$$
simplify
$$- \tilde x^{2} - 5 \tilde y^{2} + 5 = 0$$
$$\tilde x^{2} + 5 \tilde y^{2} - 5 = 0$$
Given equation is ellipse
$$\frac{\tilde x^{2}}{\left(\frac{1}{\frac{1}{5} \sqrt{5}}\right)^{2}} + \frac{\tilde y^{2}}{\left(\frac{\frac{1}{5} \sqrt{5}}{\frac{1}{5} \sqrt{5}}\right)^{2}} = 1$$
- reduced to canonical form
The center of canonical coordinate system at point O
(-1, 0)

Basis of the canonical coordinate system
$$\vec e_1 = \left( \frac{\sqrt{2}}{2}, \ \frac{\sqrt{2}}{2}\right)$$
$$\vec e_2 = \left( - \frac{\sqrt{2}}{2}, \ \frac{\sqrt{2}}{2}\right)$$
Invariants method
Given line equation of 2-order:
$$- 3 x^{2} + 4 x y - 6 x - 3 y^{2} + 4 y + 2 = 0$$
This equation looks like:
$$a_{11} x^{2} + 2 a_{12} x y + 2 a_{13} x + a_{22} y^{2} + 2 a_{23} y + a_{33} = 0$$
where
$$a_{11} = -3$$
$$a_{12} = 2$$
$$a_{13} = -3$$
$$a_{22} = -3$$
$$a_{23} = 2$$
$$a_{33} = 2$$
The invariants of the equation when converting coordinates are determinants:
$$I_{1} = a_{11} + a_{22}$$
     |a11  a12|
I2 = |        |
     |a12  a22|

$$I_{3} = \left|\begin{matrix}a_{11} & a_{12} & a_{13}\\a_{12} & a_{22} & a_{23}\\a_{13} & a_{23} & a_{33}\end{matrix}\right|$$
$$I{\left(\lambda \right)} = \left|\begin{matrix}a_{11} - \lambda & a_{12}\\a_{12} & a_{22} - \lambda\end{matrix}\right|$$
     |a11  a13|   |a22  a23|
K2 = |        | + |        |
     |a13  a33|   |a23  a33|

substitute coefficients
$$I_{1} = -6$$
     |-3  2 |
I2 = |      |
     |2   -3|

$$I_{3} = \left|\begin{matrix}-3 & 2 & -3\\2 & -3 & 2\\-3 & 2 & 2\end{matrix}\right|$$
$$I{\left(\lambda \right)} = \left|\begin{matrix}- \lambda - 3 & 2\\2 & - \lambda - 3\end{matrix}\right|$$
     |-3  -3|   |-3  2|
K2 = |      | + |     |
     |-3  2 |   |2   2|

$$I_{1} = -6$$
$$I_{2} = 5$$
$$I_{3} = 25$$
$$I{\left(\lambda \right)} = \lambda^{2} + 6 \lambda + 5$$
$$K_{2} = -25$$
Because
$$I_{2} > 0 \wedge I_{1} I_{3} < 0$$
then by line type:
this equation is of type : ellipse
Make the characteristic equation for the line:
$$- I_{1} \lambda + I_{2} + \lambda^{2} = 0$$
or
$$\lambda^{2} + 6 \lambda + 5 = 0$$
$$\lambda_{1} = -1$$
$$\lambda_{2} = -5$$
then the canonical form of the equation will be
$$\tilde x^{2} \lambda_{1} + \tilde y^{2} \lambda_{2} + \frac{I_{3}}{I_{2}} = 0$$
or
$$- \tilde x^{2} - 5 \tilde y^{2} + 5 = 0$$
$$\frac{\tilde x^{2}}{\left(\frac{1}{\frac{1}{5} \sqrt{5}}\right)^{2}} + \frac{\tilde y^{2}}{\left(\frac{\frac{1}{5} \sqrt{5}}{\frac{1}{5} \sqrt{5}}\right)^{2}} = 1$$
- reduced to canonical form