For any given Hyperbola, it's corresponding Conjugate Hyperbola can be obtained by Rotating the Hyperbola by \(90^{\circ}\) (Clockwize or Counter Clockwize) and interchanging the Lengths of it's Transverse and Conjugate Axis.
Interchanging the Lengths of Transverse and Conjugate Axis in equation (2) above we get
\(\frac{y^2}{b^2} - \frac{x^2}{a^2} =1 \) ...(3)
The equation (3) above gives the Standard Coordinate Equation for Conjugate Hyperbolas to the Hyperbolas given in equation (1) above which are Hyperbolas having their Transverse Axes Parallel to the \(Y\)-Axis, Center at Origin, Length of Semi-Transverse Axis \(b\) and Length of Semi-Conjugate Axis \(a\).
Interchanging the Lengths of Transverse and Conjugate Axis in equation (5) above we get
\(\frac{x^2}{b^2} - \frac{y^2}{a^2} =1 \) ...(6)
The equation (6) above gives the Standard Coordinate Equation for Conjugate Hyperbolas to the Hyperbolas given in equation (4) above which are Hyperbolas having their Transverse Axes Parallel to the \(X\)-Axis, Center at Origin, Length of Semi-Transverse Axis \(b\) and Length of Semi-Conjugate Axis \(a\).
The following derives the Equation of Rotated Conjugate Hyperbola from Standard Coordinate Equation of Conjugate Hyperbola given in equation (3)
Multiplying equation (3) by \(a^2b^2\) on Both Sides we get
The equation (8) above gives the Equation of the Rotated Conjugate Hyperbola having Center at Origin
Setting \(a^2\sin^2\theta - b^2\cos^2\theta =\mathbf{A_c}\), \(-(b^2 + a^2)\sin2\theta=\mathbf{B_c}\) and \(a^2\cos^2\theta - b^2 \sin^2\theta=\mathbf{C_c}\) in equation (8) above we get
Setting \(- (2A_cx_c+B_cy_c)=\mathbf{D_c}\), \(-(2C_cy_c+B_cx_c)=\mathbf{E_c}\) and \(A_c{x_c}^2+C_c{y_c}^2+B_cx_cy_c -a^2b^2=\mathbf{F_c}\) in equation (10) above we get
The equation (10) and (11) above give the Implicit Coordinate Equation of the Conjugate Hyperbola for any Hyperbola Rotated Counter Clockwise by Angle \(\theta\) with respect to Positive Direction of \(X\) Axis and having Center at \((x_c,y_c)\)
where
\(\Rightarrow P = -2A{x_c}^2-Bx_cy_c -2C{y_c}^2-Bx_cy_c\)
\(\Rightarrow P = -(2A{x_c}+By_c)x_c -(2Cy_c+Bx_c)y_c\) ...(18)
Since, as given in equation set (14) \(D= -(2A{x_c}+By_c)\) and \(E=-(2C{y_c}+Bx_c)\). Substituting this in equation (18) above we get
\(P = Dx_c + Ey_c\) ...(19)
Now, substituting the value of \(P\) from equation (19) in equation (16) we get
\(F_c = F + Dx_c + Ey_c\) ...(20)
Hence, Using equation set (15) and equation (20) above, for any Arbitrarily Rotated and Translated Hyperbola whose Implicit Equation is given by equation (10) above, the Implicit Equation of it's corresponding Conjugate Hyperbola is given as
\(-Ax^2 - Bxy - Cy^2 - Dx - Ey + F + Dx_c + Ey_c=0\) ...(21)