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Q.If x=cos⁡t,y=cos⁡mtx = \cos t, y = \cos mt, then prove that (1−x2)d2ydx2−xdydx+m2y=0(1 - x^2) \frac{d^2y}{dx^2} - x \frac{dy}{dx} + m^2y = 0.

CBSECBSE Class XII Board 2026Subjective· 5mImportance★★★★★
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We use parametric differentiation to express dydx\frac{dy}{dx} and d2ydx2\frac{d^2y}{dx^2} in terms of tt, then substitute into the given differential equation. The key is that dydx=msin⁡mtsin⁡t\frac{dy}{dx} = m \frac{\sin mt}{\sin t} and d2ydx2=mcos⁡mtsin⁡t−msin⁡mtcos⁡tsin⁡3t\frac{d^2y}{dx^2} = \frac{m \cos mt \sin t - m \sin mt \cos t}{\sin^3 t}, which simplifies to satisfy the equation identically.

When a curve is given parametrically — here x=cos⁡tx = \cos t, y=cos⁡mty = \cos mt — we cannot directly write yy as a function of xx in a simple closed form. But we can still find derivatives using the chain rule: dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}, provided dx/dt≠0dx/dt \neq 0. For the second derivative, we differentiate dydx\frac{dy}{dx} with respect to tt and then divide by dx/dtdx/dt again. This is the standard parametric second derivative formula.

The problem asks us to prove a differential equation involving yy, dy/dxdy/dx, and d2y/dx2d^2y/dx^2, with coefficients in xx. So we will compute these derivatives in terms of tt, then replace xx and yy with their parametric forms, and simplify to zero.

Let's go step by step.

  1. First derivatives with respect to tt

    Given x=cos⁡tx = \cos t, so dxdt=−sin⁡t\frac{dx}{dt} = -\sin t.

    Given y=cos⁡mty = \cos mt, so dydt=−msin⁡mt\frac{dy}{dt} = -m \sin mt.

  2. First derivative dydx\frac{dy}{dx}

    Using the parametric formula:

dydx=dy/dtdx/dt=−msin⁡mt−sin⁡t=msin⁡mtsin⁡t.\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{-m \sin mt}{-\sin t} = m \frac{\sin mt}{\sin t}.

Notice the negatives cancel neatly. This is valid wherever sin⁡t≠0\sin t \neq 0, i.e., t≠nπt \neq n\pi.

  1. Second derivative d2ydx2\frac{d^2y}{dx^2} We differentiate dydx\frac{dy}{dx} with respect to tt, then divide by dx/dtdx/dt:

d2ydx2=ddt(dydx)/dxdt.\frac{d^2y}{dx^2} = \frac{d}{dt}\left( \frac{dy}{dx} \right) \Big/ \frac{dx}{dt}.

First compute ddt(msin⁡mtsin⁡t)\frac{d}{dt}\left( m \frac{\sin mt}{\sin t} \right):

ddt(msin⁡mtsin⁡t)=m⋅(mcos⁡mt)sin⁡t−sin⁡mt(cos⁡t)sin⁡2t\frac{d}{dt}\left( m \frac{\sin mt}{\sin t} \right) = m \cdot \frac{ (m \cos mt) \sin t - \sin mt (\cos t) }{\sin^2 t}

using the quotient rule. So:

ddt(dydx)=m⋅mcos⁡mtsin⁡t−sin⁡mtcos⁡tsin⁡2t.\frac{d}{dt}\left( \frac{dy}{dx} \right) = m \cdot \frac{ m \cos mt \sin t - \sin mt \cos t }{\sin^2 t}.

Now divide by dxdt=−sin⁡t\frac{dx}{dt} = -\sin t:

d2ydx2=m(mcos⁡mtsin⁡t−sin⁡mtcos⁡t)sin⁡2t⋅1−sin⁡t=−m(mcos⁡mtsin⁡t−sin⁡mtcos⁡t)sin⁡3t.\frac{d^2y}{dx^2} = \frac{ m ( m \cos mt \sin t - \sin mt \cos t ) }{\sin^2 t} \cdot \frac{1}{-\sin t} = - \frac{ m ( m \cos mt \sin t - \sin mt \cos t ) }{\sin^3 t}.

  1. Substitute into the left-hand side of the given equation We need to verify:

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

Substitute x=cos⁡tx = \cos t, y=cos⁡mty = \cos mt, and the derivatives we found.

First, 1−x2=1−cos⁡2t=sin⁡2t1 - x^2 = 1 - \cos^2 t = \sin^2 t.

So the first term becomes:

(1−x2)d2ydx2=sin⁡2t⋅(−m(mcos⁡mtsin⁡t−sin⁡mtcos⁡t)sin⁡3t)=−m(mcos⁡mtsin⁡t−sin⁡mtcos⁡t)sin⁡t.(1 - x^2) \frac{d^2y}{dx^2} = \sin^2 t \cdot \left( - \frac{ m ( m \cos mt \sin t - \sin mt \cos t ) }{\sin^3 t} \right) = - \frac{ m ( m \cos mt \sin t - \sin mt \cos t ) }{\sin t}.

Simplify the numerator:

=−m2cos⁡mtsin⁡t−msin⁡mtcos⁡tsin⁡t=−m2cos⁡mt+msin⁡mtcos⁡tsin⁡t.= - \frac{ m^2 \cos mt \sin t - m \sin mt \cos t }{\sin t} = - m^2 \cos mt + m \frac{ \sin mt \cos t }{\sin t}. …

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