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CBSE Board Examination 2026 · Section D · 5 marks

Q34: If x=cos⁡tx = \cos t⁠, y=cos⁡mty = \cos mt⁠, prove (1−x2)y′′−xy′+m2y=0(1 - x^2)y'' - xy' + m^2y = 0

The question

If x=cos⁡tx = \cos t⁠, y=cos⁡mty = \cos mt⁠, prove that

(1−x2)d2ydx2−xdydx+m2y=0.(1 - x^2)\frac{d^2y}{dx^2} - x\frac{dy}{dx} + m^2y = 0.
Exam answer
dxdt=−sin⁡t,dydt=−msin⁡mt\frac{dx}{dt} = -\sin t,\quad \frac{dy}{dt} = -m\sin mt
Why?

xx and yy are both given in terms of a parameter tt⁠, so first differentiate each with respect to tt⁠.

By the chain rule, the inner function mtmt has derivative mm⁠:

ddtcos⁡mt=−msin⁡mt\frac{d}{dt}\cos mt = -m\sin mt
∴ dydx=dy/dtdx/dt=msin⁡mtsin⁡t\therefore\ \frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{m\sin mt}{\sin t}
Why?

For parametric equations,

dydx=dydt÷dxdt\frac{dy}{dx} = \frac{dy}{dt}\div\frac{dx}{dt}

The two minus signs cancel.

dydx=−msin⁡mt−sin⁡t=msin⁡mtsin⁡t\begin{aligned} \frac{dy}{dx} &= \frac{-m\sin mt}{-\sin t} \\ &= \frac{m\sin mt}{\sin t} \end{aligned}

Then multiply both sides by sin⁡t\sin t to get the next line.

⇒sin⁡t dydx=msin⁡mt\Rightarrow \sin t\,\frac{dy}{dx} = m\sin mt
Why?

Clearing the fraction first is a good idea: the next derivative is then a product rule instead of a quotient rule, and the working is shorter.

Differentiating both sides w.r.t. xx⁠,

sin⁡t d2ydx2+cos⁡t dtdx⋅dydx=m2cos⁡mt dtdx\begin{aligned} &\sin t\,\frac{d^2y}{dx^2} + \cos t\,\frac{dt}{dx}\cdot\frac{dy}{dx} \\ &= m^2\cos mt\,\frac{dt}{dx} \end{aligned}
Why?

The left side is a product, sin⁡t\sin t times dydx\frac{dy}{dx}⁠, so use the product rule.

sin⁡t\sin t and msin⁡mtm\sin mt are functions of tt⁠, and tt is a function of xx⁠. So by the chain rule

ddxsin⁡t=cos⁡t dtdxddx(msin⁡mt)=m2cos⁡mt dtdx\begin{aligned} \frac{d}{dx}\sin t &= \cos t\,\frac{dt}{dx} \\ \frac{d}{dx}(m\sin mt) &= m^2\cos mt\,\frac{dt}{dx} \end{aligned}

For the left side, take u=sin⁡tu = \sin t and v=dydxv = \frac{dy}{dx}⁠:

u′=cos⁡t dtdxv′=ddx(dydx)=d2ydx2(uv)′=uv′+vu′=sin⁡t d2ydx2+dydxcos⁡t dtdx\begin{aligned} u' &= \cos t\,\frac{dt}{dx} \\ v' &= \frac{d}{dx}\left(\frac{dy}{dx}\right) = \frac{d^2y}{dx^2} \\[4pt] (uv)' &= uv' + vu' \\ &= \sin t\,\frac{d^2y}{dx^2} + \frac{dy}{dx}\cos t\,\frac{dt}{dx} \end{aligned}

For the right side, msin⁡mtm\sin mt⁠: the derivative of sin⁡mt\sin mt with respect to tt is mcos⁡mtm\cos mt⁠, so m⋅mcos⁡mt=m2cos⁡mtm \cdot m\cos mt = m^2\cos mt⁠, times dtdx\frac{dt}{dx}⁠.

Putting dtdx=−1sin⁡t\frac{dt}{dx} = -\frac{1}{\sin t} and multiplying both sides by sin⁡t\sin t⁠,

sin⁡t d2ydx2−cos⁡tsin⁡t⋅dydx=−m2cos⁡mtsin⁡t\begin{aligned} &\sin t\,\frac{d^2y}{dx^2} - \frac{\cos t}{\sin t}\cdot\frac{dy}{dx} \\ &= -\frac{m^2\cos mt}{\sin t} \end{aligned} sin⁡2t d2ydx2−cos⁡t dydx=−m2cos⁡mt\sin^2t\,\frac{d^2y}{dx^2} - \cos t\,\frac{dy}{dx} = -m^2\cos mt
Why?

dtdx\frac{dt}{dx} is the reciprocal of dxdt=−sin⁡t\frac{dx}{dt} = -\sin t⁠. Putting it in gives the first line.

dtdx=1dx/dt=1−sin⁡t=−1sin⁡tcos⁡t⋅(−1sin⁡t)⋅dydx=−cos⁡tsin⁡t⋅dydxm2cos⁡mt⋅(−1sin⁡t)=−m2cos⁡mtsin⁡t\begin{aligned} \frac{dt}{dx} &= \frac{1}{dx/dt} = \frac{1}{-\sin t} = -\frac{1}{\sin t} \\[4pt] &\cos t\cdot\left(-\frac{1}{\sin t}\right)\cdot\frac{dy}{dx} \\ &= -\frac{\cos t}{\sin t}\cdot\frac{dy}{dx} \\[4pt] &m^2\cos mt\cdot\left(-\frac{1}{\sin t}\right) \\ &= -\frac{m^2\cos mt}{\sin t} \end{aligned}

Multiplying every term by sin⁡t\sin t clears the denominators. The first term becomes sin⁡2t d2ydx2\sin^2t\,\frac{d^2y}{dx^2}⁠, and in the other two terms sin⁡t\sin t cancels.

sin⁡t⋅sin⁡t d2ydx2=sin⁡2t d2ydx2sin⁡t⋅cos⁡tsin⁡t⋅dydx=cos⁡t dydxsin⁡t⋅m2cos⁡mtsin⁡t=m2cos⁡mt\begin{aligned} \sin t \cdot \sin t\,\frac{d^2y}{dx^2} &= \sin^2t\,\frac{d^2y}{dx^2} \\ \sin t \cdot \frac{\cos t}{\sin t}\cdot\frac{dy}{dx} &= \cos t\,\frac{dy}{dx} \\ \sin t \cdot \frac{m^2\cos mt}{\sin t} &= m^2\cos mt \end{aligned}

As sin⁡2t=1−cos⁡2t=1−x2\sin^2t = 1 - \cos^2t = 1 - x^2⁠, cos⁡t=x\cos t = x and cos⁡mt=y\cos mt = y⁠,

Why?

The result must be in xx and yy⁠, so replace every expression in tt⁠. Use

sin⁡2t+cos⁡2t=1\sin^2t + \cos^2t = 1

together with the given x=cos⁡tx = \cos t and y=cos⁡mty = \cos mt⁠.

sin⁡2t=1−cos⁡2t=1−x2cos⁡t=x−m2cos⁡mt=−m2y\begin{aligned} \sin^2t &= 1 - \cos^2t = 1 - x^2 \\ \cos t &= x \\ -m^2\cos mt &= -m^2y \end{aligned}
(1−x2)d2ydx2−xdydx=−m2y(1 - x^2)\frac{d^2y}{dx^2} - x\frac{dy}{dx} = -m^2y
Why?

Add m2ym^2y to both sides to get the required form with 0 on the right.

∴ (1−x2)d2ydx2−xdydx+m2y=0\therefore\ (1 - x^2)\dfrac{d^2y}{dx^2} - x\dfrac{dy}{dx} + m^2y = 0⁠. Hence proved.

Where this comes from

Chapter 5, Continuity and Differentiability: Second derivative of a parametric function.

Question type: Parametric form + Second derivative (combines 2 types)

How to spot it: click to see

Type 8. Parametric form: xx and yy given through tt or θ\theta

Spot it: two equations, one for xx and one for yy⁠, both in the same third letter.

Here: First, x=cos⁡tx = \cos t and y=cos⁡mty = \cos mt share tt⁠: divide dydt\frac{dy}{dt} by dxdt\frac{dx}{dt} to get msin⁡mtsin⁡t\frac{m\sin mt}{\sin t}⁠, and clear the fraction: sin⁡t dydx=msin⁡mt\sin t\,\frac{dy}{dx} = m\sin mt⁠.

Type 9. Second derivative: differentiate twice, then prove

Spot it: d2ydx2\frac{d^2y}{dx^2} or y′′y'' in the question, often "prove that d2ydx2+y=0\frac{d^2y}{dx^2} + y = 0".

Here: Then differentiate that again with respect to xx⁠, using dtdx=−1sin⁡t\frac{dt}{dx} = -\frac{1}{\sin t}⁠, and swap sin⁡2t\sin^2 t⁠, cos⁡t\cos t and cos⁡mt\cos mt for 1−x21 - x^2⁠, xx and yy⁠.

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