← 2017 Paper 1

UPSC 2017 Maths Optional Paper 1 Q7a — Step-by-Step Solution

16 marks · Section B

Curvature and torsion · Vector Analysis · asked 7× in 14 yrs · Read the full method →

Question

Find the curvature vector and its magnitude at any point r⃗=(θ)\vec r=(\theta) of the curve r⃗=(acos⁡θ, asin⁡θ, aθ)\vec r=(a\cos\theta,\ a\sin\theta,\ a\theta). Show that the locus of the feet of the perpendicular from the origin to the tangent is a curve that completely lies on the hyperboloid x2+y2−z2=a2x^2+y^2-z^2=a^2.

Technique

κ⃗=dT⃗/ds\vec\kappa=d\vec T/ds with constant ds/dθ=a2ds/d\theta=a\sqrt2; foot of perpendicular via λ=−(r⃗⋅r⃗ ′)/∣r⃗ ′∣2\lambda=-(\vec r\cdot\vec r\,')/|\vec r\,'|^2, then substitute into the hyperboloid.

Solution

Step 1 — Tangent and arc length

r⃗=(acos⁡θ, asin⁡θ, aθ),r⃗ ′=(−asin⁡θ, acos⁡θ, a).\vec r=(a\cos\theta,\ a\sin\theta,\ a\theta),\qquad \vec r\,'=(-a\sin\theta,\ a\cos\theta,\ a). ∣r⃗ ′∣2=a2sin⁡2θ+a2cos⁡2θ+a2=2a2 ⇒ dsdθ=a2 (constant).|\vec r\,'|^2=a^2\sin^2\theta+a^2\cos^2\theta+a^2=2a^2\ \Rightarrow\ \frac{ds}{d\theta}=a\sqrt2\ (\text{constant}).

Unit tangent

T⃗=r⃗ ′∣r⃗ ′∣=12(−sin⁡θ, cos⁡θ, 1).\vec T=\frac{\vec r\,'}{|\vec r\,'|}=\frac{1}{\sqrt2}(-\sin\theta,\ \cos\theta,\ 1).

Step 2 — Curvature vector dT⃗ds\dfrac{d\vec T}{ds}

The curvature vector is κ⃗=dT⃗ds=dT⃗/dθds/dθ\vec\kappa=\dfrac{d\vec T}{ds}=\dfrac{d\vec T/d\theta}{ds/d\theta}:

dT⃗dθ=12(−cos⁡θ, −sin⁡θ, 0),κ⃗=1a2⋅12(−cos⁡θ, −sin⁡θ, 0).\frac{d\vec T}{d\theta}=\frac{1}{\sqrt2}(-\cos\theta,\ -\sin\theta,\ 0),\qquad \vec\kappa=\frac{1}{a\sqrt2}\cdot\frac{1}{\sqrt2}(-\cos\theta,\ -\sin\theta,\ 0).   κ⃗=dT⃗ds=−12a(cos⁡θ, sin⁡θ, 0),∣κ⃗∣=κ=12a.  \boxed{\;\vec\kappa=\frac{d\vec T}{ds}=-\frac{1}{2a}\big(\cos\theta,\ \sin\theta,\ 0\big),\qquad |\vec\kappa|=\kappa=\frac{1}{2a}.\;}

The curvature is the constant 12a\dfrac{1}{2a} (as expected for a circular helix); the curvature vector points horizontally towards the axis.

Step 3 — Foot of the perpendicular from the origin to the tangent

The tangent line at parameter θ\theta is X⃗(λ)=r⃗+λr⃗ ′\vec X(\lambda)=\vec r+\lambda\vec r\,'. The foot QQ is where X⃗⋅r⃗ ′=0\vec X\cdot\vec r\,'=0 (the position vector of QQ is perpendicular to the tangent direction):

(r⃗+λr⃗ ′)⋅r⃗ ′=0 ⇒ λ=−r⃗⋅r⃗ ′∣r⃗ ′∣2.(\vec r+\lambda\vec r\,')\cdot\vec r\,'=0\ \Rightarrow\ \lambda=-\frac{\vec r\cdot\vec r\,'}{|\vec r\,'|^2}. r⃗⋅r⃗ ′=(acos⁡θ)(−asin⁡θ)+(asin⁡θ)(acos⁡θ)+(aθ)(a)=a2θ,∣r⃗ ′∣2=2a2,\vec r\cdot\vec r\,'=(a\cos\theta)(-a\sin\theta)+(a\sin\theta)(a\cos\theta)+(a\theta)(a)=a^2\theta,\qquad |\vec r\,'|^2=2a^2,

so λ=−θ2\lambda=-\dfrac{\theta}{2}. Then

Q=r⃗−θ2r⃗ ′=(acos⁡θ+θ2asin⁡θ, asin⁡θ−θ2acos⁡θ, aθ−θ2a),Q=\vec r-\frac{\theta}{2}\vec r\,'=\Big(a\cos\theta+\tfrac{\theta}{2}a\sin\theta,\ a\sin\theta-\tfrac{\theta}{2}a\cos\theta,\ a\theta-\tfrac{\theta}{2}a\Big), Q=(a2(2cos⁡θ+θsin⁡θ), a2(2sin⁡θ−θcos⁡θ), aθ2).Q=\Big(\tfrac{a}{2}(2\cos\theta+\theta\sin\theta),\ \tfrac{a}{2}(2\sin\theta-\theta\cos\theta),\ \tfrac{a\theta}{2}\Big).

Step 4 — Show QQ lies on x2+y2−z2=a2x^2+y^2-z^2=a^2

x2+y2=a24[(2cos⁡θ+θsin⁡θ)2+(2sin⁡θ−θcos⁡θ)2].x^2+y^2=\frac{a^2}{4}\Big[(2\cos\theta+\theta\sin\theta)^2+(2\sin\theta-\theta\cos\theta)^2\Big].

Expand: (2cos⁡θ+θsin⁡θ)2+(2sin⁡θ−θcos⁡θ)2=4cos⁡2θ+4θsin⁡θcos⁡θ+θ2sin⁡2θ+4sin⁡2θ−4θsin⁡θcos⁡θ+θ2cos⁡2θ=4+θ2.(2\cos\theta+\theta\sin\theta)^2+(2\sin\theta-\theta\cos\theta)^2=4\cos^2\theta+4\theta\sin\theta\cos\theta+\theta^2\sin^2\theta+4\sin^2\theta-4\theta\sin\theta\cos\theta+\theta^2\cos^2\theta=4+\theta^2. Hence

x2+y2=a24(4+θ2)=a2+a2θ24,z2=a2θ24.x^2+y^2=\frac{a^2}{4}(4+\theta^2)=a^2+\frac{a^2\theta^2}{4},\qquad z^2=\frac{a^2\theta^2}{4}. x2+y2−z2=a2+a2θ24−a2θ24=a2.x^2+y^2-z^2=a^2+\frac{a^2\theta^2}{4}-\frac{a^2\theta^2}{4}=a^2.

Answer

  x2+y2−z2=a2for all θ,  \boxed{\;x^2+y^2-z^2=a^2\quad\text{for all }\theta,\;}
We post more of this — worked solutions, CSAT trap breakdowns, guide chapters — a few times a week on Telegram. Free, no sign-in. Join

This solution is part of the Maths Coverage Map — 14 years, mapped. Get the take-away PDF free.