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JEE Main Maths Integral Calculus 2027: Standard Integrals, Substitution & Area Under Curves

The standard integral forms listed in the NTA syllabus, integration techniques, definite integral properties and area under a curve, with worked examples.

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October 1, 2026

JEE Main Maths Integral Calculus 2027: Standard Integrals, Substitution & Area Under Curves

The NTA syllabus for this chapter literally lists out a set of standard integral forms, which is a strong hint about what gets tested. Learn to recognise each pattern on sight, and a large share of Integral Calculus questions become quick lookups rather than fresh derivations.

Integration is pattern recognition. Match the integral to a standard form, and the answer follows.

Chapter at a Glance

SnapshotDetail
NTA unitUnit 8 of 14: Integral Calculus
Priority (trend-based)High
Typical question styleStandard-integral matching, definite integral property tricks and area numericals
Best first stepLearn the NTA's listed standard integral forms by sight recognition

Priority reflects past-paper trends, not an official NTA weightage.

What the NTA Syllabus Covers

  • Integral as an anti-derivative, fundamental integrals involving algebraic, trigonometric, exponential and logarithmic functions
  • Integration by substitution, by parts and by partial fractions, integration using trigonometric identities
  • Standard integrals of the listed forms: ∫dxx2±a2\int \frac{dx}{x^2 \pm a^2}, ∫dxx2±a2\int \frac{dx}{\sqrt{x^2 \pm a^2}}, ∫dxa2−x2\int \frac{dx}{a^2 - x^2}, ∫dxa2−x2\int \frac{dx}{\sqrt{a^2 - x^2}}, and the related forms with quadratics ax2+bx+cax^2 + bx + c in the denominator or under a root, and ∫a2±x2 dx\int \sqrt{a^2 \pm x^2}\,dx, ∫x2−a2 dx\int \sqrt{x^2 - a^2}\,dx
  • Fundamental theorem of calculus, properties of definite integrals, evaluation of definite integrals, areas of regions bounded by simple curves in standard forms

Master These Topics

1. The Standard Forms the NTA Syllabus Names

∫dxx2+a2=1atan⁡−1xa+C∫dxa2−x2=12aln⁡∣a+xa−x∣+C\int \frac{dx}{x^2 + a^2} = \frac{1}{a}\tan^{-1}\frac{x}{a} + C \qquad \int \frac{dx}{a^2 - x^2} = \frac{1}{2a}\ln\left\lvert\frac{a+x}{a-x}\right\rvert + C

∫dxa2−x2=sin⁡−1xa+C∫dxx2±a2=ln⁡∣x+x2±a2∣+C\int \frac{dx}{\sqrt{a^2 - x^2}} = \sin^{-1}\frac{x}{a} + C \qquad \int \frac{dx}{\sqrt{x^2 \pm a^2}} = \ln\left\lvert x + \sqrt{x^2 \pm a^2}\right\rvert + C

For denominators of the form ax2+bx+cax^2 + bx + c, complete the square first to reduce it to one of these four forms.

Worked example: ∫dxx2+4=12tan⁡−1x2+C\displaystyle\int \frac{dx}{x^2 + 4} = \frac{1}{2}\tan^{-1}\frac{x}{2} + C.

For a numerator that is linear, ∫(px+q) dxax2+bx+c\int \dfrac{(px+q)\,dx}{ax^2+bx+c}, split it into a multiple of the derivative of the denominator plus a constant, so that one part integrates to a logarithm and the other reduces to a standard form.

Worked example: ∫2x+3x2+3x+7 dx=ln⁡∣x2+3x+7∣+C\displaystyle\int \frac{2x + 3}{x^2 + 3x + 7}\,dx = \ln\lvert x^2 + 3x + 7 \rvert + C, since the numerator is exactly the derivative of the denominator.

2. Integration Techniques

  • Substitution: replace a function and its derivative with a single variable.
  • By parts: ∫u dv=uv−∫v du\displaystyle\int u\,dv = uv - \int v\,du, choosing uu using the priority order Inverse, Logarithmic, Algebraic, Trigonometric, Exponential (ILATE).
  • Partial fractions: split a rational function with a factorable denominator into simpler fractions before integrating.

Worked example (by parts): ∫xex dx=xex−∫ex dx=xex−ex+C\displaystyle\int x e^x\,dx = xe^x - \int e^x\,dx = xe^x - e^x + C.

3. Definite Integrals and a Useful Property

The fundamental theorem of calculus states ∫abf(x) dx=F(b)−F(a)\displaystyle\int_a^b f(x)\,dx = F(b) - F(a). One property saves significant work:

∫0af(x) dx=∫0af(a−x) dx\int_0^a f(x)\,dx = \int_0^a f(a - x)\,dx

Worked example: ∫0π/2sin⁡xsin⁡x+cos⁡x dx\displaystyle\int_0^{\pi/2} \frac{\sin x}{\sin x + \cos x}\,dx. Applying the property with a=π/2a = \pi/2 replaces sin⁡x\sin x with cos⁡x\cos x and vice versa. Adding the original integral II to its transformed version gives 2I=∫0π/21 dx=π/22I = \displaystyle\int_0^{\pi/2} 1\,dx = \pi/2, so I=π/4I = \pi/4.

Trap: This symmetry trick only works cleanly with limits 00 to aa (or −a-a to aa for even/odd functions). Do not force it onto arbitrary limits.

4. Area Under a Curve

The area under $y = x^2$ from $x=0$ to $x=3$ is exactly $9$, found using the fundamental theorem of calculus.
The area under $y = x^2$ from $x=0$ to $x=3$ is exactly $9$, found using the fundamental theorem of calculus.

Worked example: The area under y=x2y = x^2 from x=0x = 0 to x=3x = 3 is ∫03x2 dx=[x33]03=273=9\displaystyle\int_0^3 x^2\,dx = \left[\frac{x^3}{3}\right]_0^3 = \frac{27}{3} = 9.


Common Traps to Avoid

  • Forgetting to complete the square before matching a quadratic denominator to a standard form.
  • Applying the ILATE rule backwards, which leads to an integral that never simplifies.
  • Using the ∫0af(x)=∫0af(a−x)\int_0^a f(x) = \int_0^a f(a-x) trick with the wrong limits.
  • Leaving out the constant of integration in an indefinite integral.

60-Second Revision Sheet

  • ∫dxx2+a2=1atan⁡−1xa\int \dfrac{dx}{x^2+a^2} = \tfrac{1}{a}\tan^{-1}\tfrac{x}{a}; ∫dxa2−x2=sin⁡−1xa\int \dfrac{dx}{\sqrt{a^2-x^2}} = \sin^{-1}\tfrac{x}{a}
  • By parts: ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du (choose uu by ILATE)
  • ∫0af(x) dx=∫0af(a−x) dx\int_0^a f(x)\,dx = \int_0^a f(a-x)\,dx
  • Area under a curve: ∫aby dx\int_a^b y\,dx

Your Study Plan

  1. Day 1: standard integral forms and completing the square.
  2. Day 2: substitution, by parts and partial fractions.
  3. Day 3: definite integral properties and symmetry tricks.
  4. Day 4: area under curves and a timed mixed set.

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Frequently Asked Questions

How do I recognise which standard form an integral matches?

Look at the denominator or the expression under the square root. A sum of squares suggests tan⁡−1\tan^{-1}, a difference under a root suggests sin⁡−1\sin^{-1}, and so on.

When is the property ∫0af(x) dx=∫0af(a−x) dx\int_0^a f(x)\,dx = \int_0^a f(a-x)\,dx useful?

When adding the original integral to its transformed version cancels the hard part and leaves a simple constant integral, as in ratios of sine and cosine over symmetric limits.

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