The only critical point is the solution of the simultaneous equations
( x ) 2 + 3 x y + 2 ( y ) 2 = 0 (x)^2 +3xy+2(y)^2=0 ( x ) 2 + 3 x y + 2 ( y ) 2 = 0
4 − ( x ) 2 = 0 4-(x)^2=0 4 − ( x ) 2 = 0
x = − 2 : 4 − 6 y + 2 y 2 = 0 x=-2: 4-6y+2y^2=0 x = − 2 : 4 − 6 y + 2 y 2 = 0
y 2 − 3 y + 2 = 0 y^2-3y+2=0 y 2 − 3 y + 2 = 0
( y − 1 ) ( y − 2 ) = 0 (y-1)(y-2)=0 ( y − 1 ) ( y − 2 ) = 0
P o i n t ( − 2 , 1 ) , P o i n t ( − 2 , 2 ) Point(-2, 1), Point (-2, 2) P o in t ( − 2 , 1 ) , P o in t ( − 2 , 2 )
x = 2 : 4 + 6 y + 2 y 2 = 0 x=2: 4+6y+2y^2=0 x = 2 : 4 + 6 y + 2 y 2 = 0
y 2 + 3 y + 2 = 0 y^2+3y+2=0 y 2 + 3 y + 2 = 0
( y + 1 ) ( y + 2 ) = 0 (y+1)(y+2)=0 ( y + 1 ) ( y + 2 ) = 0
P o i n t ( 2 , − 2 ) , P o i n t ( 2 , − 1 ) Point(2, -2), Point (2, -1) P o in t ( 2 , − 2 ) , P o in t ( 2 , − 1 )
Critical points of the system
P o i n t ( − 2 , 1 ) , P o i n t ( − 2 , 2 ) , Point(-2, 1), Point (-2, 2), P o in t ( − 2 , 1 ) , P o in t ( − 2 , 2 ) ,
P o i n t ( 2 , − 2 ) , P o i n t ( 2 , − 1 ) Point(2, -2), Point (2, -1) P o in t ( 2 , − 2 ) , P o in t ( 2 , − 1 )
The Jacobian matrix is
J = ( ∂ f ∂ x ∂ f ∂ y ∂ g ∂ x ∂ g ∂ y ) = ( 2 x + 3 y 3 x + 4 y − 2 x 0 ) J=\begin{pmatrix}
\dfrac{\partial f}{\partial x} & \dfrac{\partial f}{\partial y} \\
\\
\dfrac{\partial g}{\partial x} & \dfrac{\partial g}{\partial y}
\end{pmatrix}=\begin{pmatrix}
2x+3y & 3x+4y \\
-2x & 0
\end{pmatrix} J = ⎝ ⎛ ∂ x ∂ f ∂ x ∂ g ∂ y ∂ f ∂ y ∂ g ⎠ ⎞ = ( 2 x + 3 y − 2 x 3 x + 4 y 0 )
At the P o i n t ( − 2 , 1 ) Point(-2, 1) P o in t ( − 2 , 1 ) we get the matrix ( − 1 − 2 4 0 ) \begin{pmatrix}
-1 & -2 \\
4& 0
\end{pmatrix} ( − 1 4 − 2 0 ) and so the two eigenvalues are
− 1 − i 31 2 \dfrac{-1-i\sqrt{31}}{2} 2 − 1 − i 31 and − 1 + i 31 2 . \dfrac{-1+i\sqrt{31}}{2}. 2 − 1 + i 31 .
As the eigenvalues are complex with negative real part, we get a spiral sink, which is an asymptotically stable equilibrium point.
At the P o i n t ( − 2 , 2 ) Point(-2, 2) P o in t ( − 2 , 2 ) we get the matrix ( 2 2 4 0 ) \begin{pmatrix}
2 & 2 \\
4 & 0
\end{pmatrix} ( 2 4 2 0 ) and so the two eigenvalues are − 2 -2 − 2 and 4. 4. 4.
As the eigenvalues are real and opposite signs, we get a saddle, which is an unstable equilibrium point.
At the P o i n t ( 2 , − 2 ) Point(2, -2) P o in t ( 2 , − 2 ) we get the matrix ( − 2 − 2 − 4 0 ) \begin{pmatrix}
-2 & -2 \\
-4 & 0
\end{pmatrix} ( − 2 − 4 − 2 0 ) and so the two eigenvalues are − 4 -4 − 4 and 2. 2. 2.
As the eigenvalues are real and opposite signs, we get a saddle, which is an unstable equilibrium point.
At the P o i n t ( 2 , − 1 ) Point(2, -1) P o in t ( 2 , − 1 ) we get the matrix ( 1 2 − 4 0 ) \begin{pmatrix}
1 & 2 \\
-4 & 0
\end{pmatrix} ( 1 − 4 2 0 ) and so the two eigenvalues are
1 − i 31 2 \dfrac{1-i\sqrt{31}}{2} 2 1 − i 31 and 1 + i 31 2 . \dfrac{1+i\sqrt{31}}{2}. 2 1 + i 31 .
As the eigenvalues are complex with positive real part, we get a spiral source, which is an unstable equilibrium point.
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