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Limits Continuity and Differentiability question

2025 · 28 Jan · Shift 2 · Q46
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  5. /2025 · 28 Jan · Shift 2 · Q46

Limits Continuity and Differentiability question

2025 · 28 Jan · Shift 2 · Q46

JEE MainMathematicsLimits Continuity and DifferentiabilityNumerical+4 / −1
Let f(x)=lim⁡n→∞∑r=0n(tan⁡(x/2r+1)+tan⁡3(x/2r+1)1−tan⁡2(x/2r+1))f(x)=\lim \limits_{n \rightarrow \infty} \sum\limits_{r=0}^n\left(\frac{\tan \left(x / 2^{r+1}\right)+\tan ^3\left(x / 2^{r+1}\right)}{1-\tan ^2\left(x / 2^{r+1}\right)}\right)f(x)=n→∞lim​r=0∑n​(1−tan2(x/2r+1)tan(x/2r+1)+tan3(x/2r+1)​) Then lim⁡x→0ex−ef(x)(x−f(x))\lim\limits_{x \rightarrow 0} \frac{e^x-e^{f(x)}}{(x-f(x))}x→0lim​(x−f(x))ex−ef(x)​ is equal to ‾\underline{\hspace{2cm}}​.
Numerical answer
View written solutionFree

Correct answer: 1

  1. Simplify the summand

Let

θr=x2r+1.\theta_r=\frac{x}{2^{r+1}}.θr​=2r+1x​.

Then the summand is

tan⁡θr+tan⁡3θr1−tan⁡2θr=tan⁡θr(1+tan⁡2θr)1−tan⁡2θr.\frac{\tan\theta_r+\tan^3\theta_r}{1-\tan^2\theta_r} =\frac{\tan\theta_r(1+\tan^2\theta_r)}{1-\tan^2\theta_r}.1−tan2θr​tanθr​+tan3θr​​=1−tan2θr​tanθr​(1+tan2θr​)​.

Using

and the identity

tan⁡2θ=2tan⁡θ1−tan⁡2θ,\tan 2\theta=\frac{2\tan\theta}{1-\tan^2\theta},tan2θ=1−tan2θ2tanθ​,

we get

tan⁡θ(1+tan⁡2θ)1−tan⁡2θ=tan⁡θsec⁡2θ1−tan⁡2θ.\frac{\tan\theta(1+\tan^2\theta)}{1-\tan^2\theta} =\frac{\tan\theta\sec^2\theta}{1-\tan^2\theta}.1−tan2θtanθ(1+tan2θ)​=1−tan2θtanθsec2θ​.

But it is easier to rewrite directly in sine-cosine form:

tan⁡θ+tan⁡3θ1−tan⁡2θ=tan⁡θ(1+tan⁡2θ)1−tan⁡2θ=tan⁡θsec⁡2θ1−tan⁡2θ.\frac{\tan\theta+\tan^3\theta}{1-\tan^2\theta} =\frac{\tan\theta(1+\tan^2\theta)}{1-\tan^2\theta} =\frac{\tan\theta\sec^2\theta}{1-\tan^2\theta}.1−tan2θtanθ+tan3θ​=1−tan2θtanθ(1+tan2θ)​=1−tan2θtanθsec2θ​.

Now,

tan⁡θ=sin⁡θcos⁡θ,sec⁡2θ=1cos⁡2θ,1−tan⁡2θ=cos⁡2θcos⁡2θ.\tan\theta=\frac{\sin\theta}{\cos\theta},\quad \sec^2\theta=\frac1{\cos^2\theta},\quad 1-\tan^2\theta=\frac{\cos2\theta}{\cos^2\theta}.tanθ=cosθsinθ​,sec2θ=cos2θ1​,1−tan2θ=cos2θcos2θ​.

So

tan⁡θsec⁡2θ1−tan⁡2θ=sin⁡θcos⁡θcos⁡2θ.\frac{\tan\theta\sec^2\theta}{1-\tan^2\theta} =\frac{\sin\theta}{\cos\theta\cos2\theta}.1−tan2θtanθsec2θ​=cosθcos2θsinθ​.

Using

sin⁡2θ=2sin⁡θcos⁡θ,\sin2\theta=2\sin\theta\cos\theta,sin2θ=2sinθcosθ,

this becomes

sin⁡2θ2cos⁡2θcos⁡2θ\frac{\sin2\theta}{2\cos^2\theta\cos2\theta}2cos2θcos2θsin2θ​

but the cleanest observation is:

tan⁡θ+tan⁡3θ1−tan⁡2θ=tan⁡θcos⁡2θ=sin⁡θcos⁡θcos⁡2θ.\frac{\tan\theta+\tan^3\theta}{1-\tan^2\theta} =\frac{\tan\theta}{\cos2\theta} =\frac{\sin\theta}{\cos\theta\cos2\theta}.1−tan2θtanθ+tan3θ​=cos2θtanθ​=cosθcos2θsinθ​.

Now compare with

tan⁡2θ=2tan⁡θ1−tan⁡2θ.\tan2\theta=\frac{2\tan\theta}{1-\tan^2\theta}.tan2θ=1−tan2θ2tanθ​.

Hence

tan⁡θ+tan⁡3θ1−tan⁡2θ=12tan⁡2θ (1+tan⁡2θ)\frac{\tan\theta+\tan^3\theta}{1-\tan^2\theta} =\frac{1}{2}\tan2\theta\,(1+\tan^2\theta)1−tan2θtanθ+tan3θ​=21​tan2θ(1+tan2θ)

which is still not telescoping directly. So instead, let us simplify more carefully:

Since

tan⁡θ+tan⁡3θ=tan⁡θ(1+tan⁡2θ)=tan⁡θsec⁡2θ,\tan\theta+\tan^3\theta=\tan\theta(1+\tan^2\theta)=\tan\theta\sec^2\theta,tanθ+tan3θ=tanθ(1+tan2θ)=tanθsec2θ,

and

1−tan⁡2θ=cos⁡2θcos⁡2θ,1-\tan^2\theta=\frac{\cos2\theta}{\cos^2\theta},1−tan2θ=cos2θcos2θ​,

we get

tan⁡θsec⁡2θ1−tan⁡2θ=tan⁡θ⋅1cos⁡2θ⋅cos⁡2θcos⁡2θ=tan⁡θcos⁡2θ.\frac{\tan\theta\sec^2\theta}{1-\tan^2\theta} =\tan\theta\cdot \frac{1}{\cos^2\theta}\cdot \frac{\cos^2\theta}{\cos2\theta} =\frac{\tan\theta}{\cos2\theta}.1−tan2θtanθsec2θ​=tanθ⋅cos2θ1​⋅cos2θcos2θ​=cos2θtanθ​.

Now,

tan⁡2θ=2tan⁡θ1−tan⁡2θ\tan2\theta=\frac{2\tan\theta}{1-\tan^2\theta}tan2θ=1−tan2θ2tanθ​

and

1+tan⁡2θ=sec⁡2θ.1+\tan^2\theta=\sec^2\theta.1+tan2θ=sec2θ.

A better route is to test whether this equals 12tan⁡2θ\frac12\tan2\theta21​tan2θ:

12tan⁡2θ=tan⁡θ1−tan⁡2θ,\frac12\tan2\theta=\frac{\tan\theta}{1-\tan^2\theta},21​tan2θ=1−tan2θtanθ​,

which is not our summand.

So let us proceed by series expansion near x=0x=0x=0, since the required limit is only as x→0x\to0x→0.


  1. Asymptotic expansion of the summand for small argument

Let u=x2r+1.u=\frac{x}{2^{r+1}}.u=2r+1x​. For small uuu,

tan⁡u=u+u33+O(u5),\tan u=u+\frac{u^3}{3}+O(u^5),tanu=u+3u3​+O(u5),

so

tan⁡2u=u2+O(u4),tan⁡3u=u3+O(u5).\tan^2 u=u^2+O(u^4),\qquad \tan^3 u=u^3+O(u^5).tan2u=u2+O(u4),tan3u=u3+O(u5).

Thus

tan⁡u+tan⁡3u=u+43u3+O(u5).\tan u+\tan^3 u=u+\frac{4}{3}u^3+O(u^5).tanu+tan3u=u+34​u3+O(u5).

Also,

11−tan⁡2u=1+u2+O(u4).\frac{1}{1-\tan^2u}=1+u^2+O(u^4).1−tan2u1​=1+u2+O(u4).

Therefore,

tan⁡u+tan⁡3u1−tan⁡2u=(u+43u3+O(u5))(1+u2+O(u4))=u+73u3+O(u5).\frac{\tan u+\tan^3u}{1-\tan^2u} =\left(u+\frac{4}{3}u^3+O(u^5)\right)(1+u^2+O(u^4)) =u+\frac{7}{3}u^3+O(u^5).1−tan2utanu+tan3u​=(u+34​u3+O(u5))(1+u2+O(u4))=u+37​u3+O(u5).

Hence

f(x)=∑r=0∞(x2r+1+O(x323r)).f(x)=\sum_{r=0}^{\infty}\left(\frac{x}{2^{r+1}}+O\left(\frac{x^3}{2^{3r}}\right)\right).f(x)=r=0∑∞​(2r+1x​+O(23rx3​)).

So

f(x)=x∑r=0∞12r+1+O(x3)=x+O(x3),f(x)=x\sum_{r=0}^{\infty}\frac1{2^{r+1}}+O(x^3) =x+O(x^3),f(x)=xr=0∑∞​2r+11​+O(x3)=x+O(x3),

because

∑r=0∞12r+1=1.\sum_{r=0}^{\infty}\frac1{2^{r+1}}=1.r=0∑∞​2r+11​=1.

Thus, near x=0x=0x=0,

f(x)→0andf(x)=x+O(x3).f(x)\to 0 \quad \text{and} \quad f(x)=x+O(x^3).f(x)→0andf(x)=x+O(x3).
  1. Evaluate the required limit

We need

L=lim⁡x→0ex−ef(x)x−f(x).L=\lim_{x\to0}\frac{e^x-e^{f(x)}}{x-f(x)}.L=x→0lim​x−f(x)ex−ef(x)​.

Apply the Mean Value Theorem to ete^tet between t=xt=xt=x and t=f(x)t=f(x)t=f(x):

ex−ef(x)=eξx(x−f(x))e^x-e^{f(x)}=e^{\xi_x}(x-f(x))ex−ef(x)=eξx​(x−f(x))

for some ξx\xi_xξx​ lying between xxx and f(x)f(x)f(x). Since both x→0x\to0x→0 and f(x)→0f(x)\to0f(x)→0, we have ξx→0\xi_x\to0ξx​→0. Therefore,

L=lim⁡x→0eξx=e0=1.L=\lim_{x\to0} e^{\xi_x}=e^0=1.L=x→0lim​eξx​=e0=1.

So the required integer is

1.\boxed{1}.1​.
  1. Comparison with stored answer

Stored correct answer = 111.

Our derived answer = 111.

Hence they agree.

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