Quick Recap — Limits: the Basics

  • A limit describes the value f(x)f(x) approaches as x→ax\to a; it exists iff the left- and right-hand limits are equal.
  • Standard limits: lim⁡x→0sin⁡xx=1\displaystyle\lim_{x\to0}\frac{\sin x}{x}=1, lim⁡x→0tan⁡xx=1\displaystyle\lim_{x\to0}\frac{\tan x}{x}=1, lim⁡x→01−cos⁡xx2=12\displaystyle\lim_{x\to0}\frac{1-\cos x}{x^2}=\tfrac12.
  • lim⁡x→0ex−1x=1\displaystyle\lim_{x\to0}\frac{e^x-1}{x}=1, lim⁡x→0ax−1x=ln⁡a\displaystyle\lim_{x\to0}\frac{a^x-1}{x}=\ln a, lim⁡x→0ln⁡(1+x)x=1\displaystyle\lim_{x\to0}\frac{\ln(1+x)}{x}=1.
  • lim⁡x→axn−anx−a=n an−1\displaystyle\lim_{x\to a}\frac{x^n-a^n}{x-a}=n\,a^{n-1}, and lim⁡x→∞(1+1x)x=e\displaystyle\lim_{x\to\infty}\Big(1+\tfrac1x\Big)^x=e.

Beyond-NCERT JEE Formulae

L'Hopital's Rule. When lim⁡x→af(x)g(x)\displaystyle\lim_{x\to a}\dfrac{f(x)}{g(x)} has the indeterminate form 00\dfrac00 or ∞∞\dfrac{\infty}{\infty}, the limit equals the ratio of the derivatives:

lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x),\lim_{x\to a}\dfrac{f(x)}{g(x)}=\lim_{x\to a}\dfrac{f'(x)}{g'(x)},

provided the latter limit exists, and the step may be repeated as long as the indeterminate form persists. [JEE Tip] L'Hopital is a fast alternative to Taylor-series expansion for 00\dfrac00 and ∞∞\dfrac{\infty}{\infty} limits. [JEE Tip] Differentiate the numerator and the denominator SEPARATELY -- do NOT apply the quotient rule.

Newton-Leibniz Rule. To differentiate an integral whose limits depend on xx,

ddx∫g(x)h(x)f(t) dt=f(h(x)) h′(x)−f(g(x)) g′(x).\dfrac{d}{dx}\int_{g(x)}^{h(x)}f(t)\,dt=f\big(h(x)\big)\,h'(x)-f\big(g(x)\big)\,g'(x).

Evaluate the integrand at each limit and multiply by that limit's derivative; the antiderivative of ff is never needed.

Handy Limit Forms.

  • lim⁡x→0(1+ax)1/x=ea\displaystyle\lim_{x\to0}(1+ax)^{1/x}=e^{a}, which generalises the definition of ee.
  • lim⁡x→0tan⁡−1xx=1\displaystyle\lim_{x\to0}\dfrac{\tan^{-1}x}{x}=1, and likewise lim⁡x→0sin⁡−1xx=1\displaystyle\lim_{x\to0}\dfrac{\sin^{-1}x}{x}=1.
  • lim⁡x→0ax−bxx=ln⁡ab\displaystyle\lim_{x\to0}\dfrac{a^{x}-b^{x}}{x}=\ln\dfrac{a}{b} for a,b>0a,b>0.

Differentiability Shortcuts.

  • ∣f(x)∣|f(x)| is NOT differentiable where f(x)=0f(x)=0 and ff changes sign (a simple root); at a double root, where ff keeps its sign, ∣f∣|f| stays smooth.
  • max⁡{u,v}\max\{u,v\} and min⁡{u,v}\min\{u,v\} of two differentiable functions have corners only at crossings, where the graphs meet with different slopes.

Solved Examples — Beyond-NCERT Formulae

Each example applies one of the Beyond-NCERT tools above; several are cross-checked by a second method.

Example 1 — A 00\dfrac00 limit by L'Hopital, cross-checked by series

Evaluate lim⁡x→0x−sin⁡xx3\displaystyle\lim_{x\to0}\dfrac{x-\sin x}{x^{3}}.

L'Hopital. The form is 00\dfrac00, so differentiate numerator and denominator separately (never as a quotient):

lim⁡x→0x−sin⁡xx3=lim⁡x→01−cos⁡x3x2=lim⁡x→0sin⁡x6x=16.\lim_{x\to0}\dfrac{x-\sin x}{x^{3}}=\lim_{x\to0}\dfrac{1-\cos x}{3x^{2}}=\lim_{x\to0}\dfrac{\sin x}{6x}=\dfrac16.

Each stage stays 00\dfrac00 until the last, where sin⁡x6x→16\dfrac{\sin x}{6x}\to\dfrac16.

Series cross-check. From sin⁡x=x−x36+⋯\sin x=x-\dfrac{x^{3}}{6}+\cdots, the numerator is x−sin⁡x=x36−⋯x-\sin x=\dfrac{x^{3}}{6}-\cdots, so dividing by x3x^{3} again gives 16\dfrac16. Both routes agree.

Example 2 — An ∞∞\dfrac{\infty}{\infty} limit by repeated L'Hopital

Evaluate lim⁡x→∞x2ex\displaystyle\lim_{x\to\infty}\dfrac{x^{2}}{e^{x}}.

The form is ∞∞\dfrac{\infty}{\infty}. Apply L'Hopital and repeat while the form persists:

lim⁡x→∞x2ex=lim⁡x→∞2xex=lim⁡x→∞2ex=0.\lim_{x\to\infty}\dfrac{x^{2}}{e^{x}}=\lim_{x\to\infty}\dfrac{2x}{e^{x}}=\lim_{x\to\infty}\dfrac{2}{e^{x}}=0.

The exponential outgrows any power of xx, so the limit is 00.

Example 3 — Newton-Leibniz with one variable limit

Find ddx∫0x2sin⁡t dt\dfrac{d}{dx}\displaystyle\int_{0}^{x^{2}}\sin t\,dt.

Here the lower limit is g(x)=0g(x)=0 with g′(x)=0g'(x)=0, the upper limit is h(x)=x2h(x)=x^{2} with h′(x)=2xh'(x)=2x, and the integrand is f(t)=sin⁡tf(t)=\sin t. The Newton-Leibniz rule gives

ddx∫0x2sin⁡t dt=sin⁡ ⁣(x2)⋅2x−sin⁡(0)⋅0=2xsin⁡ ⁣(x2).\dfrac{d}{dx}\int_{0}^{x^{2}}\sin t\,dt=\sin\!\big(x^{2}\big)\cdot 2x-\sin(0)\cdot 0=2x\sin\!\big(x^{2}\big).

Cross-check. Integrating first, ∫0x2sin⁡t dt=[−cos⁡t]0x2=1−cos⁡ ⁣(x2)\displaystyle\int_{0}^{x^{2}}\sin t\,dt=\big[-\cos t\big]_{0}^{x^{2}}=1-\cos\!\big(x^{2}\big), whose derivative is indeed 2xsin⁡ ⁣(x2)2x\sin\!\big(x^{2}\big).

Example 4 — Newton-Leibniz with both limits variable

Find ddx∫xx3et2 dt\dfrac{d}{dx}\displaystyle\int_{x}^{x^{3}}e^{t^{2}}\,dt.

Now the lower limit is g(x)=xg(x)=x with g′(x)=1g'(x)=1, the upper limit is h(x)=x3h(x)=x^{3} with h′(x)=3x2h'(x)=3x^{2}, and the integrand is f(t)=et2f(t)=e^{t^{2}}. The upper limit contributes f(h) h′f(h)\,h' while the lower limit subtracts f(g) g′f(g)\,g':

ddx∫xx3et2 dt=e(x3)2⋅3x2−ex2⋅1=3x2ex6−ex2.\dfrac{d}{dx}\int_{x}^{x^{3}}e^{t^{2}}\,dt=e^{(x^{3})^{2}}\cdot 3x^{2}-e^{x^{2}}\cdot 1=3x^{2}e^{x^{6}}-e^{x^{2}}.

Notice that the antiderivative of et2e^{t^{2}}, which is not elementary, is never required.

Example 5 — A handy exponential form, with a log-and-L'Hopital check

Evaluate lim⁡x→0(1+3x)1/x\displaystyle\lim_{x\to0}(1+3x)^{1/x}.

This matches the standard form lim⁡x→0(1+ax)1/x=ea\displaystyle\lim_{x\to0}(1+ax)^{1/x}=e^{a} with a=3a=3, so the value is e3e^{3}.

Cross-check by logarithm and L'Hopital. Put L=lim⁡x→0(1+3x)1/xL=\displaystyle\lim_{x\to0}(1+3x)^{1/x}. Taking logs turns the power into a 00\dfrac00 quotient:

ln⁡L=lim⁡x→0ln⁡(1+3x)x=lim⁡x→03/(1+3x)1=3,\ln L=\lim_{x\to0}\dfrac{\ln(1+3x)}{x}=\lim_{x\to0}\dfrac{3/(1+3x)}{1}=3,

so L=e3L=e^{3}, confirming the shortcut.

Example 6 — A 1∞1^{\infty} form via logarithm and L'Hopital

Evaluate lim⁡x→0(cos⁡x)1/x2\displaystyle\lim_{x\to0}(\cos x)^{1/x^{2}}.

The base tends to 11 while the exponent tends to ∞\infty, a genuine 1∞1^{\infty} form. Set L=lim⁡x→0(cos⁡x)1/x2L=\displaystyle\lim_{x\to0}(\cos x)^{1/x^{2}} and take logarithms:

ln⁡L=lim⁡x→0ln⁡cos⁡xx2.\ln L=\lim_{x\to0}\dfrac{\ln\cos x}{x^{2}}.

The right side is 00\dfrac00, so by L'Hopital,

ln⁡L=lim⁡x→0−tan⁡x2x=−12,\ln L=\lim_{x\to0}\dfrac{-\tan x}{2x}=-\dfrac12,

using tan⁡xx→1\dfrac{\tan x}{x}\to1. Hence L=e−1/2L=e^{-1/2}.

Example 7 — Handy inverse-trig and difference-of-powers forms

Evaluate lim⁡x→07x−3xx\displaystyle\lim_{x\to0}\dfrac{7^{x}-3^{x}}{x} first. Applying lim⁡x→0ax−bxx=ln⁡ab\displaystyle\lim_{x\to0}\dfrac{a^{x}-b^{x}}{x}=\ln\dfrac{a}{b} with a=7a=7 and b=3b=3,

lim⁡x→07x−3xx=ln⁡73.\lim_{x\to0}\dfrac{7^{x}-3^{x}}{x}=\ln\dfrac{7}{3}.

Next evaluate lim⁡x→0tan⁡−15xsin⁡−12x\displaystyle\lim_{x\to0}\dfrac{\tan^{-1}5x}{\sin^{-1}2x}. Using tan⁡−15x5x→1\dfrac{\tan^{-1}5x}{5x}\to1 together with sin⁡−12x2x→1\dfrac{\sin^{-1}2x}{2x}\to1, the numerator behaves like 5x5x while the denominator behaves like 2x2x:

lim⁡x→0tan⁡−15xsin⁡−12x=52.\lim_{x\to0}\dfrac{\tan^{-1}5x}{\sin^{-1}2x}=\dfrac{5}{2}.