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Concept 12 / 14Coordinate Geometry

Rotation of Axes and Identifying Conics from the General Second-Degree Equation

Translation and rotation of coordinate axes, the angle tan 2 theta = 2h/(a - b) that removes the xy term, the discriminant h^2 - ab and the determinant Delta for classifying ax^2 + 2hxy + by^2 + 2gx + 2fy + c = 0 as a pair of lines, circle, parabola, ellipse or hyperbola, and invariants under rotation.

Figure 1
The general second-degree equation ax2+2hxy+by2+2gx+2fy+c=0ax^{2} + 2hxy + by^{2} + 2gx + 2fy + c = 0 always represents a conic (possibly degenerate). The standard forms studied earlier have their axes along the coordinate axes; a general equation can be brought to standard form by moving and turning the axes. Translation of axes. Moving the origin to (h0,k0)(h_{0}, k_{0}) with parallel axes: x=X+h0x = X + h_{0}, y=Y+k0y = Y + k_{0}. Choosing (h0,k0)(h_{0}, k_{0}) at the centre of a central conic removes the linear terms. The centre is found by solving ax+hy+g=0ax + hy + g = 0 and hx+by+f=0hx + by + f = 0 (the partial derivatives of the left side set to zero). Rotation of axes. Turning the axes through an angle θ\theta about the origin: x=Xcos⁡θ−Ysin⁡θx = X\cos\theta - Y\sin\theta, y=Xsin⁡θ+Ycos⁡θy = X\sin\theta + Y\cos\theta. Substituting into ax2+2hxy+by2ax^{2} + 2hxy + by^{2}, the coefficient of XYXY vanishes when tan⁡2θ=2ha−b\tan 2\theta = \frac{2h}{a - b} (and θ=π4\theta = \frac{\pi}{4} if a=ba = b). Rotating by this angle aligns the new axes with the axes of the conic, as the figure shows for x2−xy+y2=3x^{2} - xy + y^{2} = 3, which becomes X26+Y22=1\frac{X^{2}}{6} + \frac{Y^{2}}{2} = 1 after a 45∘45^{\circ} rotation. Invariants. Under rotation, a+ba + b and ab−h2ab - h^{2} do not change, and neither does cc (or the determinant Δ\Delta below). So after rotation the new coefficients a′,b′a', b' of X2,Y2X^{2}, Y^{2} are the roots of λ2−(a+b)λ+(ab−h2)=0\lambda^{2} - (a + b)\lambda + (ab - h^{2}) = 0: they are the eigenvalues of the matrix [ahhb]\begin{bmatrix} a & h \\ h & b \end{bmatrix}. This gives the standard form without performing the substitution. Classification. Let Δ=∣ahghbfgfc∣=abc+2fgh−af2−bg2−ch2\Delta = \begin{vmatrix} a & h & g \\ h & b & f \\ g & f & c \end{vmatrix} = abc + 2fgh - af^{2} - bg^{2} - ch^{2}. If Δ=0\Delta = 0: a degenerate conic, i.e. a pair of straight lines (real and intersecting if h2>abh^{2} > ab, parallel or coincident if h2=abh^{2} = ab, or a single point if h2<abh^{2} < ab). If Δ≠0\Delta \neq 0: h2<abh^{2} < ab: an ellipse (a circle if also a=ba = b and h=0h = 0), or no real locus. h2=abh^{2} = ab: a parabola. h2>abh^{2} > ab: a hyperbola; a rectangular hyperbola if in addition a+b=0a + b = 0. The quantity h2−abh^{2} - ab plays the role of a discriminant, exactly like B2−4ACB^{2} - 4AC for the quadratic form. It is invariant under rotation, which is why the type of a conic does not depend on how it is tilted. Eccentricity from the invariants. For a central conic, once a′,b′a', b' are known the standard form gives ee directly. For example, if after translation and rotation the equation is X26+Y22=1\frac{X^{2}}{6} + \frac{Y^{2}}{2} = 1, then e=1−26=23e = \sqrt{1 - \frac{2}{6}} = \sqrt{\frac{2}{3}}. Conics as focus-directrix loci. A locus defined by 'distance to a point == ee times distance to a line' can be written directly: (x−α)2+(y−β)2=e2(lx+my+n)2l2+m2(x - \alpha)^{2} + (y - \beta)^{2} = e^{2}\frac{(lx + my + n)^{2}}{l^{2} + m^{2}}. Expanding gives a general second-degree equation whose type depends only on ee (ellipse, parabola, hyperbola for e<1e < 1, =1= 1, >1> 1). Key Takeaways: - Centre: solve ax+hy+g=0ax + hy + g = 0 and hx+by+f=0hx + by + f = 0. - Rotation removing xyxy: tan⁡2θ=2ha−b\tan 2\theta = \frac{2h}{a - b} (θ=45∘\theta = 45^{\circ} if a=ba = b). - Invariants: a+ba + b, ab−h2ab - h^{2}, Δ\Delta; new X2,Y2X^{2}, Y^{2} coefficients are the roots of λ2−(a+b)λ+(ab−h2)=0\lambda^{2} - (a + b)\lambda + (ab - h^{2}) = 0. - Δ=0\Delta = 0: pair of lines. Δ≠0\Delta \neq 0: ellipse if h2<abh^{2} < ab, parabola if h2=abh^{2} = ab, hyperbola if h2>abh^{2} > ab. - Rectangular hyperbola: h2>abh^{2} > ab and a+b=0a + b = 0. - Circle: a=ba = b, h=0h = 0. - Pitfall: reading hh as the coefficient of xyxy instead of half of it. Brain-Teaser 1: Identify the conic x2+4xy+4y2−3x−6=0x^{2} + 4xy + 4y^{2} - 3x - 6 = 0. Solution: a=1a = 1, h=2h = 2, b=4b = 4, g=−32g = -\frac{3}{2}, f=0f = 0, c=−6c = -6. Then h2−ab=4−4=0h^{2} - ab = 4 - 4 = 0. Δ=abc+2fgh−af2−bg2−ch2=−24+0−0−9+24=−9≠0\Delta = abc + 2fgh - af^{2} - bg^{2} - ch^{2} = -24 + 0 - 0 - 9 + 24 = -9 \neq 0. So it is a parabola. Note that the quadratic part (x+2y)2(x + 2y)^{2} is a perfect square, which is the characteristic sign of a parabola: its axis is parallel to x+2y=0x + 2y = 0. Brain-Teaser 2: Reduce 5x2+4xy+8y2=365x^{2} + 4xy + 8y^{2} = 36 to standard form and find its eccentricity. Solution: a=5a = 5, h=2h = 2, b=8b = 8, so h2−ab=4−40<0h^{2} - ab = 4 - 40 < 0: an ellipse. The new coefficients are roots of λ2−13λ+36=0\lambda^{2} - 13\lambda + 36 = 0, i.e. 44 and 99. So the standard form is 4X2+9Y2=364X^{2} + 9Y^{2} = 36, or X29+Y24=1\frac{X^{2}}{9} + \frac{Y^{2}}{4} = 1. Then e=1−49=53e = \sqrt{1 - \frac{4}{9}} = \frac{\sqrt{5}}{3}. The rotation angle satisfies tan⁡2θ=45−8=−43\tan 2\theta = \frac{4}{5 - 8} = -\frac{4}{3}, but the invariants gave the shape without computing it. Brain-Teaser 3: For what λ\lambda does x2+λxy+y2−5x−7y+6=0x^{2} + \lambda xy + y^{2} - 5x - 7y + 6 = 0 represent a pair of straight lines? Solution: Here a=b=1a = b = 1, h=λ2h = \frac{\lambda}{2}, g=−52g = -\frac{5}{2}, f=−72f = -\frac{7}{2}, c=6c = 6. Setting Δ=0\Delta = 0: abc+2fgh−af2−bg2−ch2=6+2(−72)(−52)λ2−494−254−6λ24=0abc + 2fgh - af^{2} - bg^{2} - ch^{2} = 6 + 2(-\frac{7}{2})(-\frac{5}{2})\frac{\lambda}{2} - \frac{49}{4} - \frac{25}{4} - 6\frac{\lambda^{2}}{4} = 0. That is, 6+35λ4−744−3λ22=06 + \frac{35\lambda}{4} - \frac{74}{4} - \frac{3\lambda^{2}}{2} = 0; multiply by 44: 24+35λ−74−6λ2=024 + 35\lambda - 74 - 6\lambda^{2} = 0, so 6λ2−35λ+50=06\lambda^{2} - 35\lambda + 50 = 0, giving λ=52\lambda = \frac{5}{2} or λ=103\lambda = \frac{10}{3}. Check λ=52\lambda = \frac{5}{2}: the quadratic part x2+52xy+y2=(x+2y)(x+y2)x^{2} + \frac{5}{2}xy + y^{2} = (x + 2y)(x + \frac{y}{2}), and indeed (x+2y−3)(x+y2−2)(x + 2y - 3)(x + \frac{y}{2} - 2) expands to the given equation.