Mister Exam

2xy+2xz+2yz canonical form

The teacher will be very surprised to see your correct solution 😉

v

The graph:

x: [, ]
y: [, ]
z: [, ]

Quality:

 (Number of points on the axis)

Plot type:

The solution

You have entered [src]
2*x*y + 2*x*z + 2*y*z = 0
2xy+2xz+2yz=02 x y + 2 x z + 2 y z = 0
2*x*y + 2*x*z + 2*y*z = 0
Invariants method
Given equation of the surface of 2-order:
2xy+2xz+2yz=02 x y + 2 x z + 2 y z = 0
This equation looks like:
a11x2+2a12xy+2a13xz+2a14x+a22y2+2a23yz+2a24y+a33z2+2a34z+a44=0a_{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
a11=0a_{11} = 0
a12=1a_{12} = 1
a13=1a_{13} = 1
a14=0a_{14} = 0
a22=0a_{22} = 0
a23=1a_{23} = 1
a24=0a_{24} = 0
a33=0a_{33} = 0
a34=0a_{34} = 0
a44=0a_{44} = 0
The invariants of the equation when converting coordinates are determinants:
I1=a11+a22+a33I_{1} = a_{11} + a_{22} + a_{33}
     |a11  a12|   |a22  a23|   |a11  a13|
I2 = |        | + |        | + |        |
     |a12  a22|   |a23  a33|   |a13  a33|

I3=a11a12a13a12a22a23a13a23a33I_{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|
I4=a11a12a13a14a12a22a23a24a13a23a33a34a14a24a34a44I_{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(λ)=a11λa12a13a12a22λa23a13a23a33λI{\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
I1=0I_{1} = 0
     |0  1|   |0  1|   |0  1|
I2 = |    | + |    | + |    |
     |1  0|   |1  0|   |1  0|

I3=011101110I_{3} = \left|\begin{matrix}0 & 1 & 1\\1 & 0 & 1\\1 & 1 & 0\end{matrix}\right|
I4=0110101011000000I_{4} = \left|\begin{matrix}0 & 1 & 1 & 0\\1 & 0 & 1 & 0\\1 & 1 & 0 & 0\\0 & 0 & 0 & 0\end{matrix}\right|
I(λ)=λ111λ111λI{\left(\lambda \right)} = \left|\begin{matrix}- \lambda & 1 & 1\\1 & - \lambda & 1\\1 & 1 & - \lambda\end{matrix}\right|
     |0  0|   |0  0|   |0  0|
K2 = |    | + |    | + |    |
     |0  0|   |0  0|   |0  0|

     |0  1  0|   |0  1  0|   |0  1  0|
     |       |   |       |   |       |
K3 = |1  0  0| + |1  0  0| + |1  0  0|
     |       |   |       |   |       |
     |0  0  0|   |0  0  0|   |0  0  0|

I1=0I_{1} = 0
I2=3I_{2} = -3
I3=2I_{3} = 2
I4=0I_{4} = 0
I(λ)=λ3+3λ+2I{\left(\lambda \right)} = - \lambda^{3} + 3 \lambda + 2
K2=0K_{2} = 0
K3=0K_{3} = 0
Because
I3 != 0

then by type of surface:
you need to
Make the characteristic equation for the surface:
I1λ2+I2λI3+λ3=0- I_{1} \lambda^{2} + I_{2} \lambda - I_{3} + \lambda^{3} = 0
or
λ33λ2=0\lambda^{3} - 3 \lambda - 2 = 0
λ1=2\lambda_{1} = 2
λ2=1\lambda_{2} = -1
λ3=1\lambda_{3} = -1
then the canonical form of the equation will be
(z~2λ3+(x~2λ1+y~2λ2))+I4I3=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
2x~2y~2z~2=02 \tilde x^{2} - \tilde y^{2} - \tilde z^{2} = 0
x~2(22)2+(y~212+z~212)=0- \frac{\tilde x^{2}}{\left(\frac{\sqrt{2}}{2}\right)^{2}} + \left(\frac{\tilde y^{2}}{1^{2}} + \frac{\tilde z^{2}}{1^{2}}\right) = 0
this equation is fora type cone
- reduced to canonical form