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11.3 Unified Properties of Conic Sections and Trajectory Problems

Key Takeaways

  • All non-degenerate conic sections can be defined by a single unified focus-directrix relation: the locus of points P where the ratio of distance to focus F to distance to directrix l is constant eccentricity e = |PF| / d(P, l).

  • If e < 1, the locus is an ellipse; if e = 1, a parabola; if e > 1, a hyperbola.

  • The unified polar coordinate equation with pole at focus is r = ep / (1 - e cos θ), unifying all three curves into a single parametric family.

  • The four foundational methods for solving trajectory (locus) problems in Gaokao are the Definition Method, Direct Algebraic Method, Related Point Method, and Parameter Elimination Method.

  • Line-conic intersection problems require constructing a quadratic system, checking the discriminant Δ > 0, applying Vieta's formulas, and verifying geometric constraints (e.g. slope existence, asymptote parallelism).

Last updated: July 2026

11.3 Unified Properties of Conic Sections and Trajectory Problems

In high school mathematics and the Gaokao examination, conic sections are unified under a single geometric definition involving a focus, a directrix, and eccentricity ee. Trajectory (locus) problems represent one of the most challenging problem types in analytic geometry, testing students' ability to translate geometric conditions into algebraic equations and manipulate quadratic systems.


1. The Unified Focus-Directrix Definition

Any non-degenerate conic section (ellipse, parabola, or hyperbola) can be defined as the locus of a point P(x,y)P(x, y) moving in a plane such that the ratio of its distance from a fixed point FF (the focus) to its distance from a fixed line ll (the directrix, where F∉lF \notin l) is a constant non-negative real number ee (the eccentricity).

∣PF∣d(P,l)=e\frac{|PF|}{d(P, l)} = e
Eccentricity RangeConic Section TypeGeometric Shape CharacteristicsDirectrix Distance from Center (for Ellipse/Hyperbola)
0<e<10 < e < 1EllipseClosed curve around focusd=a2cd = \dfrac{a^2}{c}
e=1e = 1ParabolaOpen single-branch curved=p2d = \dfrac{p}{2} from vertex
e>1e > 1HyperbolaOpen two-branch curved=a2cd = \dfrac{a^2}{c}

Unified Polar Equation: Setting the pole at the focus FF and polar axis along the axis of symmetry towards the directrix, the unified equation for all conic sections is: r=ep1−ecos⁡θr = \frac{ep}{1 - e \cos \theta}

  • When e<1e < 1, the denominator 1−ecos⁡θ>01 - e \cos \theta > 0 for all θ\theta, giving a bounded closed ellipse.
  • When e=1e = 1, 1−cos⁡θ=01 - \cos \theta = 0 at θ=0\theta = 0, giving an unbounded parabola.
  • When e>1e > 1, 1−ecos⁡θ=01 - e \cos \theta = 0 at cos⁡θ=1e\cos \theta = \frac{1}{e}, producing two asymptotic directions of a hyperbola.

2. Four Systematic Methods for Trajectory (Locus) Determination

Solving trajectory problems in the Gaokao requires identifying which of the four standard algebraic strategies applies to the geometric condition provided.

Method 1: Definition Method (定义法)

Strategy: Examine the geometric condition given in the problem statement. If it matches a known canonical definition of a conic section, directly identify the curve type and compute its parameters (a,b,c,a, b, c, or pp).

  • Ellipse: ∣PF1∣+∣PF2∣=2a>2c|PF_1| + |PF_2| = 2a > 2c
  • Hyperbola: ∣∣PF1∣−∣PF2∣∣=2a<2c\bigl||PF_1| - |PF_2|\bigr| = 2a < 2c
  • Parabola: ∣PF∣=d(P,l)|PF| = d(P, l)

Method 2: Direct Algebraic Method (直译法)

Strategy: Set up a Cartesian coordinate system, assign coordinates P(x,y)P(x, y) to the moving point, express the given geometric relations directly as an equation f(x,y)=0f(x, y) = 0, and simplify algebraically while taking care to state domain restrictions (xx or yy bounds).

Method 3: Related Point / Transfer Method (相关点法 / 代入法)

Strategy: When the trajectory of point P(x,y)P(x,y) depends on the motion of another point Q(x0,y0)Q(x_0, y_0) that moves along a known curve C:g(x0,y0)=0C: g(x_0, y_0) = 0:

  1. Express x0x_0 and y0y_0 in terms of xx and yy: x0=h1(x,y)x_0 = h_1(x, y) and y0=h2(x,y)y_0 = h_2(x, y).
  2. Substitute (x0,y0)(x_0, y_0) into the known curve equation g(h1(x,y),h2(x,y))=0g(h_1(x,y), h_2(x,y)) = 0.
  3. Simplify to obtain the desired trajectory equation for P(x,y)P(x, y).

Method 4: Parameter Elimination Method (参数法)

Strategy: Express the coordinates P(x,y)P(x, y) of the moving point in terms of an auxiliary parameter tt (such as slope kk, angle θ\theta, or time tt):

{x=f(t)y=g(t)\begin{cases} x = f(t) \\ y = g(t) \end{cases}

Eliminate tt between the two parametric equations to obtain the Cartesian equation F(x,y)=0F(x, y) = 0, ensuring the range of tt correctly translates into the domain/range of xx and yy.


3. Advanced Algebraic Techniques for Line-Conic Intersections

When a line l:y=kx+ml: y = kx + m (or x=my+nx = my + n) intersects a conic section C:Ax2+By2=1C: Ax^2 + By^2 = 1, Gaokao problems systematically test the Delta-Vieta System:

  1. Substitution & Quadratic Reduction: Substitute y=kx+my = kx + m into the conic equation to obtain a standard single-variable quadratic equation: Ax2+B(kx+m)2=1  ⟹  (A+Bk2)x2+2BKmx+(Bm2−1)=0Ax^2 + B(kx + m)^2 = 1 \implies (A + B k^2)x^2 + 2BKmx + (Bm^2 - 1) = 0
  2. Coefficient Non-Zero Check: Verify that the quadratic coefficient A+Bk2≠0A + Bk^2 \neq 0.
    • Caution: If A+Bk2=0A + Bk^2 = 0, the line is parallel to an asymptote of a hyperbola, resulting in at most one intersection point!
  3. Discriminant Constraint (Δ>0\Delta > 0): Compute Δ=(2BKm)2−4(A+Bk2)(Bm2−1)>0\Delta = (2BKm)^2 - 4(A + Bk^2)(Bm^2 - 1) > 0 to guarantee two real distinct intersection points M(x1,y1)M(x_1, y_1) and N(x2,y2)N(x_2, y_2).
  4. Vieta's Formulas: Express x1+x2x_1 + x_2 and x1x2x_1 x_2 in terms of parameters kk and mm.
  5. Point-Subtraction Method (点差法) for Midpoint Chords: If M(x1,y1)M(x_1, y_1) and N(x2,y2)N(x_2, y_2) lie on x2a2±y2b2=1\frac{x^2}{a^2} \pm \frac{y^2}{b^2} = 1 with chord midpoint P0(x0,y0)P_0(x_0, y_0): x12−x22a2±y12−y22b2=0  ⟹  kchord⋅kOP0=∓b2a2\frac{x_1^2 - x_2^2}{a^2} \pm \frac{y_1^2 - y_2^2}{b^2} = 0 \implies k_{\text{chord}} \cdot k_{OP_0} = \mp \frac{b^2}{a^2}

4. Worked Gaokao Exam Examples

Example 1: Trajectory of a Moving Circle Center (Definition Method)

Problem: A moving circle MM is externally tangent to circle C1:(x+2)2+y2=1C_1: (x+2)^2 + y^2 = 1 and internally tangent to circle C2:(x−2)2+y2=25C_2: (x-2)^2 + y^2 = 25. Find the trajectory equation of the center M(x,y)M(x, y) of the moving circle.

Solution:

  1. Circle C1C_1 has center F1(−2,0)F_1(-2, 0) and radius R1=1R_1 = 1. Circle C2C_2 has center F2(2,0)F_2(2, 0) and radius R2=5R_2 = 5.
  2. Let rr be the radius of the moving circle MM.
  3. External tangency to C1  ⟹  ∣MF1∣=r+R1=r+1C_1 \implies |MF_1| = r + R_1 = r + 1.
  4. Internal tangency to C2  ⟹  ∣MF2∣=R2−r=5−rC_2 \implies |MF_2| = R_2 - r = 5 - r.
  5. Adding the two distance equations: ∣MF1∣+∣MF2∣=(r+1)+(5−r)=6|MF_1| + |MF_2| = (r + 1) + (5 - r) = 6
  6. Notice that ∣F1F2∣=4|F_1F_2| = 4. Since ∣MF1∣+∣MF2∣=6>∣F1F2∣=4|MF_1| + |MF_2| = 6 > |F_1F_2| = 4, by the definition of an ellipse, the locus of MM is an ellipse with foci F1(−2,0)F_1(-2, 0) and F2(2,0)F_2(2, 0).
  7. Here 2a=6  ⟹  a=32a = 6 \implies a = 3, and c=2c = 2. Thus b2=a2−c2=9−4=5b^2 = a^2 - c^2 = 9 - 4 = 5.
  8. The trajectory equation of MM is x29+y25=1\dfrac{x^2}{9} + \dfrac{y^2}{5} = 1.

Example 2: Trajectory by Related Point Method

Problem: A point Q(x0,y0)Q(x_0, y_0) moves along the parabola y2=4xy^2 = 4x. Point P(x,y)P(x, y) divides the segment OQOQ (where OO is the origin) such that OP⃗=23OQ⃗\vec{OP} = \frac{2}{3}\vec{OQ}. Find the equation of the trajectory of PP.

Solution:

  1. Express the vector relation in coordinates: (x,y)=23(x0,y0)  ⟹  x=23x0,y=23y0(x, y) = \frac{2}{3}(x_0, y_0) \implies x = \frac{2}{3}x_0, \quad y = \frac{2}{3}y_0
  2. Solve for x0x_0 and y0y_0 in terms of xx and yy: x0=32x,y0=32yx_0 = \frac{3}{2}x, \quad y_0 = \frac{3}{2}y
  3. Since Q(x0,y0)Q(x_0, y_0) lies on y2=4xy^2 = 4x, substitute (x0,y0)(x_0, y_0) into y02=4x0y_0^2 = 4x_0: (32y)2=4(32x)  ⟹  94y2=6x\left(\frac{3}{2}y\right)^2 = 4\left(\frac{3}{2}x\right) \implies \frac{9}{4}y^2 = 6x
  4. Multiply both sides by 49\frac{4}{9}: y2=249x=83xy^2 = \frac{24}{9}x = \frac{8}{3}x
  5. The trajectory of point PP is the parabola y2=83xy^2 = \dfrac{8}{3}x.
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Flowchart for Selecting Trajectory Determination Methods in Gaokao
Test Your Knowledge

According to the unified focus-directrix definition of conic sections, a curve has a focus at F(1,0) and a directrix x = 4. If the eccentricity of the curve is e = 1/2, what type of conic section is it and what is its standard equation?

A

Ellipse with standard equation x^2/4 + y^2/3 = 1

B

Hyperbola with standard equation x^2/4 - y^2/3 = 1

C

Ellipse with standard equation x^2/3 + y^2/4 = 1

D

Parabola with standard equation y^2 = 4x

Test Your Knowledge

A point P(x, y) moves such that its distance to point A(-3, 0) minus its distance to point B(3, 0) is equal to 4, i.e., |PA| - |PB| = 4. What is the exact trajectory of point P?

A

The right branch of the hyperbola x^2/4 - y^2/5 = 1

B

The entire hyperbola x^2/4 - y^2/5 = 1

C

The left branch of the hyperbola x^2/4 - y^2/5 = 1

D

An ellipse with equation x^2/9 + y^2/5 = 1

Test Your Knowledge

A straight line l: y = x + m and the hyperbola C: x^2 - y^2 = 2 intersect at two distinct points M and N. What is the set of possible values for the real parameter m?

A

Ø (empty set, no such real number m exists)

B

m ∈ (-√2, √2)

C

m ∈ (-∞, ∞)

D

m ≠ 0

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