Indeterminate forms

At a Glance

Why This Chapter Matters

Indeterminate-form limits appear in Section A compulsory (Q1), always for 10 marks. All four historical examples involve exponential forms (1∞1^\infty, ∞0\infty^0) or a product (0⋅∞0\cdot\infty). The technique is always the same: take logarithm to convert the exponent to a product, then evaluate the resulting 0⋅∞0\cdot\infty limit by substitution or L’Hôpital. The answers are always clean numbers like e2/πe^{2/\pi}, e−1e^{-1}, or ee.

Minimum Theory

The indeterminate forms that appear on UPSC:

FormExampleStrategy
1∞1^\infty(tan⁡x)tan⁡2x(\tan x)^{\tan 2x} as x→π/4x\to\pi/4Take ln⁡L=lim⁡(exponent)⋅ln⁡(base)\ln L = \lim (\text{exponent})\cdot\ln(\text{base})
∞0\infty^0(ex+x)1/x(e^x+x)^{1/x} as x→∞x\to\inftyTake ln⁡L=lim⁡ln⁡(base)exponent−1\ln L = \lim \frac{\ln(\text{base})}{\text{exponent}^{-1}}
0⋅∞0\cdot\infty(1−z)tan⁡πz2(1-z)\tan\frac{\pi z}{2} as z→1z\to1Rewrite as 01/∞\frac{0}{1/\infty} or substitute z=1+hz=1+h

Indeterminate form types and the logarithm strategy

Toolkit. After taking logarithm, the limit reduces to evaluating something of the form lim⁡f(h)/g(h)\lim f(h)/g(h) as h→0h\to 0, where both ff and gg vanish. Two methods work:

Key identity. tan⁡ ⁣(π2+θ)=−cot⁡θ\tan\!\left(\dfrac\pi2+\theta\right) = -\cot\theta. This converts tan⁡(π/2+ε)\tan(\pi/2+\varepsilon) (which blows up) into −cot⁡ε-\cot\varepsilon (which has a finite small-ε\varepsilon expansion). It appears in three of the four historical problems.

Question Archetypes

ArchetypeRecognition
indeterminate-form-limitEvaluate a limit of the form 1∞1^\infty, ∞0\infty^0, or 0⋅∞0\cdot\infty; answer via logarithm + substitution

indeterminate-form-limit (4 question(s); 2015, 2018, 2020, 2022)

Recognition Cues

Solution Template

  1. Substitute the limit point; identify which indeterminate form appears.
  2. Take ln⁡L=lim⁡(exponent)⋅ln⁡(base)\ln L = \lim(\text{exponent})\cdot\ln(\text{base}) (for 1∞1^\infty or ∞0\infty^0).
  3. Shift to a small-parameter hh: let x=x0+hx = x_0 + h or x=1/tx = 1/t; use tan⁡(π/2+h)=−cot⁡h\tan(\pi/2+h) = -\cot h.
  4. Expand ln⁡(1+u)≈u\ln(1+u)\approx u and sin⁡θ≈θ\sin\theta\approx\theta (or apply L’Hôpital if cleaner).
  5. Exponentiate: L=eln⁡LL = e^{\ln L}.

Worked Example 1

2020 Paper 1, 2020-P1-Q1c (10 marks)

Evaluate lim⁡x→π/4(tan⁡x)tan⁡2x\lim_{x\to\pi/4}(\tan x)^{\tan 2x}.

Step 1. At x=π/4x=\pi/4: tan⁡x→1\tan x\to 1, tan⁡2x→∞\tan 2x\to\infty. Form: 1∞1^\infty.

Step 2. ln⁡L=lim⁡x→π/4tan⁡2x⋅ln⁡(tan⁡x)\ln L = \lim_{x\to\pi/4}\tan 2x\cdot\ln(\tan x).

Step 3. Let x=π/4+tx = \pi/4 + t, t→0t\to 0. Then tan⁡2x=tan⁡(π/2+2t)=−cot⁡2t\tan 2x = \tan(\pi/2+2t) = -\cot 2t. Using tan⁡(π/4+t)=(1+tan⁡t)/(1−tan⁡t)\tan(\pi/4+t)=(1+\tan t)/(1-\tan t), for small tt: ln⁡(tan⁡x)=ln⁡1+t+O(t3)1−t+O(t3)≈ln⁡(1+2t)≈2t.\ln(\tan x) = \ln\frac{1+t+O(t^3)}{1-t+O(t^3)} \approx \ln(1+2t) \approx 2t.

Step 4. −cot⁡2t≈−1/(2t)-\cot 2t\approx -1/(2t). Product: tan⁡2x⋅ln⁡(tan⁡x)≈−12t⋅2t=−1.\tan 2x\cdot\ln(\tan x) \approx -\frac{1}{2t}\cdot 2t = -1.

Step 5. L=e−1=1/e.\boxed{L = e^{-1} = 1/e.}

(L’Hôpital check: ln⁡L=lim⁡ln⁡tan⁡xcot⁡2x\ln L = \lim\dfrac{\ln\tan x}{\cot 2x}; differentiate: 2/sin⁡2x−2/sin⁡22x=−sin⁡2x∣x=π/4=−1\dfrac{2/\sin 2x}{-2/\sin^2 2x} = -\sin 2x\big|_{x=\pi/4} = -1 ✓.)

Worked Example 2

2015 Paper 1, 2015-P1-Q1c (10 marks)

Evaluate lim⁡x→a(2−xa)tan⁡(πx/2a)\lim_{x\to a}\bigl(2-\dfrac{x}{a}\bigr)^{\tan(\pi x/2a)}.

Step 1. At x=ax=a: base =1=1, exponent =tan⁡(π/2)=±∞=\tan(\pi/2)=\pm\infty. Form: 1∞1^\infty.

Step 2. ln⁡L=lim⁡x→atan⁡ ⁣(πx2a)ln⁡ ⁣(2−xa)\ln L = \lim_{x\to a}\tan\!\left(\frac{\pi x}{2a}\right)\ln\!\left(2-\frac{x}{a}\right).

Step 3. Let x=a+hx=a+h; then 2−x/a=1−h/a2-x/a = 1-h/a and tan⁡(π/2+πh/2a)=−cot⁡(πh/2a)\tan(\pi/2+\pi h/2a)=-\cot(\pi h/2a).

Step 4. Using ln⁡(1−h/a)≈−h/a\ln(1-h/a)\approx -h/a and cot⁡(πh/2a)≈2a/(πh)\cot(\pi h/2a)\approx 2a/(\pi h): ln⁡L=lim⁡h→0(−2aπh) ⁣(−ha)=2π.\ln L = \lim_{h\to 0}\left(-\frac{2a}{\pi h}\right)\!\left(-\frac{h}{a}\right) = \frac{2}{\pi}.

Step 5. L=e2/π.\boxed{L = e^{2/\pi}.}

Worked Example 3

2018 Paper 1, 2018-P1-Q1c (10 marks)

Does lim⁡z→1(1−z)tan⁡ ⁣(πz2)\lim_{z\to1}(1-z)\tan\!\left(\dfrac{\pi z}{2}\right) exist? Find its value.

Step 1. At z=1z=1: (1−z)→0(1-z)\to0 and tan⁡(π/2)→±∞\tan(\pi/2)\to\pm\infty. Form: 0⋅∞0\cdot\infty.

Step 2. Let z=1+hz=1+h; then 1−z=−h1-z=-h and tan⁡(π/2+πh/2)=−cot⁡(πh/2)\tan(\pi/2+\pi h/2)=-\cot(\pi h/2).

Step 3. Product =(−h)⋅(−cot⁡(πh/2))=hcot⁡(πh/2)=hcos⁡(πh/2)sin⁡(πh/2)= (-h)\cdot(-\cot(\pi h/2)) = h\cot(\pi h/2) = \dfrac{h\cos(\pi h/2)}{\sin(\pi h/2)}.

Step 4. Using sin⁡(πh/2)≈πh/2\sin(\pi h/2)\approx\pi h/2: product ≈h⋅1πh/2=2π\approx\dfrac{h\cdot 1}{\pi h/2} = \dfrac{2}{\pi}.

Step 5. The two-sided limit exists: L=2/π.\boxed{L = 2/\pi.}

Worked Example 4

2022 Paper 1, 2022-P1-Q1c (10 marks)

Evaluate lim⁡x→∞(ex+x)1/x\lim_{x\to\infty}(e^x+x)^{1/x}.

Step 1. At x→∞x\to\infty: base →∞\to\infty, exponent →0\to 0. Form: ∞0\infty^0.

Step 2. ln⁡L=lim⁡x→∞ln⁡(ex+x)x\ln L = \lim_{x\to\infty}\dfrac{\ln(e^x+x)}{x}.

Step 3. Factor exe^x: ln⁡(ex+x)=x+ln⁡(1+xe−x)\ln(e^x+x) = x + \ln(1+xe^{-x}).

Step 4. As x→∞x\to\infty, xe−x→0xe^{-x}\to 0, so ln⁡(1+xe−x)→0\ln(1+xe^{-x})\to 0. Thus ln⁡L=1\ln L = 1.

Step 5. L=e.\boxed{L = e.}

Common Traps

Marks-Aware Writing

All four questions are 10 marks. Show: (a) the indeterminate form identified, (b) the logarithm step ln⁡L=…\ln L = \ldots, (c) the substitution or asymptotics, (d) the limiting value of ln⁡L\ln L, (e) the final answer L=e(…)L = e^{(\ldots)}. Each step earns 2 marks. Writing “by L’Hôpital the answer is…” without showing the differentiation earns 2–3 marks at most.

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