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Exercise 9.4 · Q25

Q.Evaluate the following limit:
[!FORMULA] lim⁡x→0ex−e−xsin⁡x\lim_{x\to0}\dfrac{e^x-e^{-x}}{\sin x}

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Concept understanding — Standard Limits

A Toolkit of Named Limits

Some limits recur so often across problems that it is worth memorising their values outright, along with the one theorem that proves the trickiest of them: the Sandwich (Squeeze) Theorem.

The Sandwich Theorem

Theorem 9.5. If g(x)≤f(x)≤h(x)g(x) \le f(x) \le h(x) for all xx near x0x_0 (except possibly at x0x_0 itself), and if

lim⁡x→x0g(x)=lim⁡x→x0h(x)=l,\lim_{x\to x_0} g(x) = \lim_{x\to x_0} h(x) = l,

then lim⁡x→x0f(x)=l\lim_{x\to x_0} f(x) = l too — ff is "squeezed" between two functions that agree in the limit, so it has no room to do anything else.

Illustration: to show lim⁡x→0x2sin⁡ ⁣1x2=0\displaystyle\lim_{x\to 0} x^2\sin\!\frac{1}{x^2} = 0, note that sin⁡(⋅)\sin(\cdot) is always between −1-1 and 11, so −x2≤x2sin⁡1x2≤x2-x^2 \le x^2\sin\frac{1}{x^2} \le x^2. Since both −x2-x^2 and x2x^2 tend to 00 as x→0x\to 0, the Sandwich Theorem forces the middle expression to 00 as well — even though lim⁡x→0sin⁡1x2\lim_{x\to 0}\sin\frac{1}{x^2} on its own does not exist (it oscillates wildly), so the product rule alone could never have been applied directly.

Watch out

This is exactly why the Sandwich Theorem is indispensable rather than a curiosity: whenever one factor oscillates without a limit but is bounded, and the other factor is squeezed to zero, the ordinary product law (Concept 2) is not applicable — you need the sandwich.

The two flagship trigonometric limits

Result 9.1.

(a)lim⁡θ→0sin⁡θθ=1(b)lim⁡θ→01−cos⁡θθ=0\text{(a)}\quad \lim_{\theta\to 0}\frac{\sin\theta}{\theta} = 1 \qquad\qquad \text{(b)}\quad \lim_{\theta\to 0}\frac{1-\cos\theta}{\theta} = 0

Part (a) is proved geometrically by sandwiching sin⁡θθ\frac{\sin\theta}{\theta} between cos⁡θ\cos\theta and 11 using the areas of a triangle, a sector, and a larger triangle built on the unit circle; since both bounding functions tend to 11 as θ→0\theta\to0, so must sin⁡θθ\frac{\sin\theta}{\theta}. Part (b) follows algebraically from (a) by writing 1−cos⁡θ=2sin⁡2θ21-\cos\theta = 2\sin^2\frac{\theta}{2} and splitting the quotient into a sin⁡\sin-over-argument piece (which uses part (a)) times a factor that vanishes.

A direct corollary worth keeping separate: lim⁡x→0sin⁡x=0\displaystyle\lim_{x\to 0}\sin x = 0, obtained from the sandwich −∣x∣≤sin⁡x≤∣x∣-|x|\le \sin x \le |x|.

The full standard-limit toolkit (§9.2.10)

Alongside the trig pair above, these are worth having on instant recall — none require anything beyond algebra and substitution to use (their proofs, where given, lean on the exponential/log relationship or on the trig pair):

lim⁡x→0ex−1x=1lim⁡x→0ax−1x=log⁡a (a>0)lim⁡x→0log⁡(1+x)x=1\lim_{x\to 0}\frac{e^x-1}{x}=1 \qquad\quad \lim_{x\to 0}\frac{a^x-1}{x}=\log a \ (a>0) \qquad\quad \lim_{x\to 0}\frac{\log(1+x)}{x}=1

lim⁡x→0sin⁡−1xx=1lim⁡x→0tan⁡−1xx=1\lim_{x\to 0}\frac{\sin^{-1}x}{x}=1 \qquad\quad \lim_{x\to 0}\frac{\tan^{-1}x}{x}=1

And the three equivalent forms of the number ee as a limit:

lim⁡x→∞(1+1x)x=elim⁡x→0(1+x)1/x=elim⁡x→∞(1+kx)x=ek\lim_{x\to\infty}\left(1+\frac{1}{x}\right)^x = e \qquad\quad \lim_{x\to 0}(1+x)^{1/x} = e \qquad\quad \lim_{x\to\infty}\left(1+\frac{k}{x}\right)^x = e^k

Note

ee is a transcendental number — it never satisfies any polynomial equation with rational coefficients. That's part of why it shows up as a genuinely new limiting constant here rather than something expressible in simpler closed form.

The recognise-and-substitute pattern

Nearly every "hard-looking" limit in this section is really one of the above standard forms in disguise, reached via a clean substitution y=(some expression in x)y = (\text{some expression in } x) chosen so that y→0y \to 0 (or y→∞y\to\infty) exactly when xx does. The book's worked examples all follow this shape:

  1. Spot the shell. Identify which standard form the expression resembles — a (1+□)1/□\left(1+\Box\right)^{1/\Box} shape signals ee; a sin⁡(□)□\dfrac{\sin(\Box)}{\Box} shape signals Result 9.1(a); a a□−1□\dfrac{a^{\Box}-1}{\Box} shape signals Result 9.3.
  2. Substitute yy for the "□\Box" so the expression matches the standard form exactly, tracking what y→y \to as x→x0x \to x_0.
  3. Apply the standard limit to the yy-expression, then (if the exponent or coefficient outside doesn't vanish) combine using the power/product rules from Concept 2. …

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