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Exercise 5.6 · Q8

Q.Find dydx\frac{dy}{dx} in the following: x=a(cos⁡t+log⁡tan⁡t2),y=asin⁡tx = a \left(\cos t + \log \tan \frac{t}{2}\right), y = a \sin t

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Appeared in past exams:COMEDK 2025· Set 2025-E· 1mreworded
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We use parametric differentiation: differentiate xx and yy with respect to tt, then compute dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}. The result simplifies to dydx=tan⁡t\frac{dy}{dx} = \tan t.

When a curve is given in parametric form — x=f(t)x = f(t), y=g(t)y = g(t) — the derivative dydx\frac{dy}{dx} is not directly available. But the chain rule gives a clean path:

dydx=dy/dtdx/dt,provided dxdt≠0.\frac{dy}{dx} = \frac{dy/dt}{dx/dt}, \quad \text{provided } \frac{dx}{dt} \neq 0.

This is the core idea of parametric differentiation. Instead of eliminating tt (which is often messy), we differentiate each equation with respect to the parameter tt and then take the ratio.

Let’s apply this to the given equations.


  1. Differentiate y=asin⁡ty = a \sin t with respect to tt. Since aa is a constant,

dydt=acos⁡t.\frac{dy}{dt} = a \cos t.

  1. Differentiate x=a(cos⁡t+log⁡tan⁡t2)x = a \left( \cos t + \log \tan \frac{t}{2} \right) with respect to tt. Factor out the constant aa:

dxdt=a(ddt[cos⁡t]+ddt[log⁡tan⁡t2]).\frac{dx}{dt} = a \left( \frac{d}{dt}[\cos t] + \frac{d}{dt}\left[ \log \tan \frac{t}{2} \right] \right).

The derivative of cos⁡t\cos t is −sin⁡t-\sin t.

For the logarithmic term, use the chain rule:

ddt[log⁡tan⁡t2]=1tan⁡t2⋅ddt[tan⁡t2].\frac{d}{dt} \left[ \log \tan \frac{t}{2} \right] = \frac{1}{\tan \frac{t}{2}} \cdot \frac{d}{dt}\left[ \tan \frac{t}{2} \right].

Now ddt[tan⁡t2]=sec⁡2t2⋅12\frac{d}{dt}\left[ \tan \frac{t}{2} \right] = \sec^2 \frac{t}{2} \cdot \frac{1}{2} (by the chain rule again, since derivative of t2\frac{t}{2} is 12\frac{1}{2}).

So

ddt[log⁡tan⁡t2]=1tan⁡t2⋅12sec⁡2t2.\frac{d}{dt} \left[ \log \tan \frac{t}{2} \right] = \frac{1}{\tan \frac{t}{2}} \cdot \frac{1}{2} \sec^2 \frac{t}{2}.

Recall that 1tan⁡θ=cot⁡θ\frac{1}{\tan \theta} = \cot \theta and sec⁡2θ=1+tan⁡2θ\sec^2 \theta = 1 + \tan^2 \theta, but here a simpler simplification is:

1tan⁡t2⋅sec⁡2t2=cos⁡t2sin⁡t2⋅1cos⁡2t2=1sin⁡t2cos⁡t2.\frac{1}{\tan \frac{t}{2}} \cdot \sec^2 \frac{t}{2} = \frac{\cos \frac{t}{2}}{\sin \frac{t}{2}} \cdot \frac{1}{\cos^2 \frac{t}{2}} = \frac{1}{\sin \frac{t}{2} \cos \frac{t}{2}}.

And sin⁡t2cos⁡t2=12sin⁡t\sin \frac{t}{2} \cos \frac{t}{2} = \frac{1}{2} \sin t (using the double-angle identity sin⁡2θ=2sin⁡θcos⁡θ\sin 2\theta = 2 \sin \theta \cos \theta).

Therefore,

1sin⁡t2cos⁡t2=2sin⁡t.\frac{1}{\sin \frac{t}{2} \cos \frac{t}{2}} = \frac{2}{\sin t}.

Including the factor 12\frac{1}{2} from earlier:

ddt[log⁡tan⁡t2]=12⋅2sin⁡t=1sin⁡t.\frac{d}{dt} \left[ \log \tan \frac{t}{2} \right] = \frac{1}{2} \cdot \frac{2}{\sin t} = \frac{1}{\sin t}. …

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