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UPSC Maths 2013 Paper 1 Q4c — Solution

20 marks · Section A

Question

A variable generator meets two generators of the system through the extremities BB and BB' of the minor axis of the principal elliptic section of the hyperboloid x2a2+y2b2z2c2=1\dfrac{x^{2}}{a^{2}}+\dfrac{y^{2}}{b^{2}}-z^{2}c^{2}=1 in PP and PP'. Prove that BPBP=a2+c2BP\cdot B'P'=a^{2}+c^{2}.

(Note: the PDF writes "z2c2z^{2}c^{2}"; the standard reading is z2/c2z^{2}/c^{2} — i.e. the standard hyperboloid of one sheet. We adopt the standard form.)

Technique

Standard ruled-surface parametrisation; the two families of generators of a hyperboloid of one sheet; explicit parametric intersection calculations.

Solution

Strategy. Identify the two ruled-line families of the hyperboloid; pick the two “fixed” generators through BB and BB' in one family; the variable generator from the other family meets both, with intersection points P,PP,P'. Compute distances.

Step 1 — Two ruled families

Rewrite the hyperboloid as

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

This yields two families of lines (rulings):

Family Λ\Lambda (parameter λ\lambda):

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

Family MM (parameter μ\mu):

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

Step 2 — Generators through BB and BB'

B=(0,b,0),  B=(0,b,0)B=(0,b,0),\;B'=(0,-b,0) are endpoints of the minor axis of the principal ellipse (which is the z=0z=0 section, the ellipse x2/a2+y2/b2=1x^{2}/a^{2}+y^{2}/b^{2}=1; minor axis is along yy when a>ba>b, with endpoints (0,±b,0)(0,\pm b,0)).

At BB (substitute y=by=b, 1+y/b=21+y/b=2, 1y/b=01-y/b=0): family MM with μ0\mu\to 0 gives the line {y=b,  x/a=z/c}\{y=b,\;x/a=z/c\}. Direction (a,0,c)(a,0,c). Call this LBL_B.

At BB' (substitute y=by=-b, 1+y/b=01+y/b=0, 1y/b=21-y/b=2): family MM with μ\mu\to\infty gives the line {y=b,  x/a=z/c}\{y=-b,\;x/a=-z/c\}. Direction (a,0,c)(a,0,-c). Call this LBL_{B'}.

Both LBL_B and LBL_{B'} are in family MM — “two generators of the same system through BB and BB'.” They are skew (different yy-values, not parallel — direction (a,0,c)(a,0,c) vs (a,0,c)(a,0,-c)).

Step 3 — Variable generator from family Λ\Lambda meets both

Take λ\ell_\lambda, the family-Λ\Lambda generator at parameter λ\lambda. We compute its intersection with LBL_B and LBL_{B'}.

Intersection P=λLBP=\ell_\lambda\cap L_B: at y=by=b, so 1y/b=0,  1+y/b=21-y/b=0,\;1+y/b=2. Plug into the family-Λ\Lambda equations:

x/az/c=0,x/a+z/c=2/λ.x/a-z/c=0,\qquad x/a+z/c=2/\lambda.

So x/a=z/c=1/λx/a=z/c=1/\lambda, giving

P=(a/λ,  b,  c/λ).P=\bigl(a/\lambda,\;b,\;c/\lambda\bigr).

Intersection P=λLBP'=\ell_\lambda\cap L_{B'}: at y=by=-b, so 1y/b=2,  1+y/b=01-y/b=2,\;1+y/b=0. Plug into family-Λ\Lambda:

x/az/c=2λ,x/a+z/c=0.x/a-z/c=2\lambda,\qquad x/a+z/c=0.

So x/a=λ,  z/c=λx/a=\lambda,\;z/c=-\lambda, giving

P=(aλ,  b,  cλ).P'=\bigl(a\lambda,\;-b,\;-c\lambda\bigr).

Step 4 — Compute BPBP and BPB'P'

BP=PB=(a/λ,  0,  c/λ)\overrightarrow{BP}=P-B=\bigl(a/\lambda,\;0,\;c/\lambda\bigr).

BP2=a2λ2+0+c2λ2=a2+c2λ2    BP=a2+c2λ.BP^{2}=\frac{a^{2}}{\lambda^{2}}+0+\frac{c^{2}}{\lambda^{2}}=\frac{a^{2}+c^{2}}{\lambda^{2}}\;\Longrightarrow\;BP=\frac{\sqrt{a^{2}+c^{2}}}{|\lambda|}.

BP=PB=(aλ,  0,  cλ)\overrightarrow{B'P'}=P'-B'=(a\lambda,\;0,\;-c\lambda).

BP2=a2λ2+c2λ2=(a2+c2)λ2    BP=λa2+c2.B'P'^{2}=a^{2}\lambda^{2}+c^{2}\lambda^{2}=(a^{2}+c^{2})\lambda^{2}\;\Longrightarrow\;B'P'=|\lambda|\sqrt{a^{2}+c^{2}}.

Step 5 — Product

BPBP=a2+c2λλa2+c2=a2+c2.BP\cdot B'P'=\frac{\sqrt{a^{2}+c^{2}}}{|\lambda|}\cdot|\lambda|\sqrt{a^{2}+c^{2}}=a^{2}+c^{2}.

Answer

  BPBP=a2+c2.  \boxed{\;BP\cdot B'P'=a^{2}+c^{2}.\;}

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