← 2014 Paper 1

UPSC 2014 Maths Optional Paper 1 Q4c — Step-by-Step Solution

15 marks · Section A

Hyperboloid of one sheet · Analytic Geometry · asked 3× in 14 yrs · Read the full method →

Question

Find the equations of the two generating lines through any point (acos⁡θ, bsin⁡θ, 0)(a\cos\theta,\,b\sin\theta,\,0) of the principal elliptic section x2a2+y2b2=1,  z=0\dfrac{x^{2}}{a^{2}}+\dfrac{y^{2}}{b^{2}}=1,\;z=0, of the hyperboloid by the plane z=0z=0.

Technique

Standard two-family factorisation of hyperboloid; substitute the point to find the parameter λ\lambda or μ\mu of each generator; compute direction.

Solution

Strategy. The hyperboloid of one sheet x2a2+y2b2−z2c2=1\dfrac{x^{2}}{a^{2}}+\dfrac{y^{2}}{b^{2}}-\dfrac{z^{2}}{c^{2}}=1 has two ruling families. Through each point of the principal section, one line of each family passes. Identify the parameters of each line; then write line equations.

Step 1 — Ruling families

Factor the hyperboloid:

(xa−zc) ⁣(xa+zc)=(1−yb) ⁣(1+yb).\left(\dfrac{x}{a}-\dfrac{z}{c}\right)\!\left(\dfrac{x}{a}+\dfrac{z}{c}\right)=\left(1-\dfrac{y}{b}\right)\!\left(1+\dfrac{y}{b}\right).

Family Λ\Lambda (parameter λ\lambda):

xa−zc=λ ⁣(1−yb),xa+zc=1λ ⁣(1+yb).\dfrac{x}{a}-\dfrac{z}{c}=\lambda\!\left(1-\dfrac{y}{b}\right),\quad\dfrac{x}{a}+\dfrac{z}{c}=\dfrac{1}{\lambda}\!\left(1+\dfrac{y}{b}\right).

Family MM (parameter μ\mu):

xa−zc=μ ⁣(1+yb),xa+zc=1μ ⁣(1−yb).\dfrac{x}{a}-\dfrac{z}{c}=\mu\!\left(1+\dfrac{y}{b}\right),\quad\dfrac{x}{a}+\dfrac{z}{c}=\dfrac{1}{\mu}\!\left(1-\dfrac{y}{b}\right).

Step 2 — Determine λ,μ\lambda,\mu at P=(acos⁡θ,bsin⁡θ,0)P=(a\cos\theta,b\sin\theta,0)

At PP: x/a=cos⁡θx/a=\cos\theta, y/b=sin⁡θy/b=\sin\theta, z/c=0z/c=0.

Substitute into family-Λ\Lambda first equation: cos⁡θ=λ(1−sin⁡θ)⇒λ=cos⁡θ1−sin⁡θ\cos\theta=\lambda(1-\sin\theta)\Rightarrow\lambda=\dfrac{\cos\theta}{1-\sin\theta}.

Substitute into family-MM first equation: cos⁡θ=μ(1+sin⁡θ)⇒μ=cos⁡θ1+sin⁡θ\cos\theta=\mu(1+\sin\theta)\Rightarrow\mu=\dfrac{\cos\theta}{1+\sin\theta}.

(Verify the second equation in each family holds — it does, by the identity cos⁡2θ=(1−sin⁡θ)(1+sin⁡θ)\cos^{2}\theta=(1-\sin\theta)(1+\sin\theta).)

Step 3 — Direction vectors of the two generators

For a line of family Λ\Lambda, parameter λ\lambda, the direction vector (proportional to ∂/∂y\partial/\partial y) works out to be (after computation):

d⃗Λ∝(a(1−λ2),  2bλ,  c(1+λ2)).\vec d_\Lambda\propto\bigl(a(1-\lambda^{2}),\;2b\lambda,\;c(1+\lambda^{2})\bigr).

Substituting λ=cos⁡θ/(1−sin⁡θ)\lambda=\cos\theta/(1-\sin\theta) and simplifying (using 1−λ2=−2sin⁡θ/(1−sin⁡θ)1-\lambda^{2}=-2\sin\theta/(1-\sin\theta) and 1+λ2=2/(1−sin⁡θ)1+\lambda^{2}=2/(1-\sin\theta)):

d⃗Λ∝(−asin⁡θ,  bcos⁡θ,  c).\vec d_\Lambda\propto\bigl(-a\sin\theta,\;b\cos\theta,\;c\bigr).

Similarly for family MM:

d⃗M∝(−asin⁡θ,  bcos⁡θ,  −c).\vec d_M\propto\bigl(-a\sin\theta,\;b\cos\theta,\;-c\bigr).

Step 4 — Line equations through PP

Generator from family Λ\Lambda:

  x−acos⁡θ−asin⁡θ=y−bsin⁡θbcos⁡θ=zc.  \boxed{\;\dfrac{x-a\cos\theta}{-a\sin\theta}=\dfrac{y-b\sin\theta}{b\cos\theta}=\dfrac{z}{c}.\;}

Generator from family MM:

Answer

  x−acos⁡θ−asin⁡θ=y−bsin⁡θbcos⁡θ=z−c.  \boxed{\;\dfrac{x-a\cos\theta}{-a\sin\theta}=\dfrac{y-b\sin\theta}{b\cos\theta}=\dfrac{z}{-c}.\;}
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