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MHT-CET Maths · Formula sheet

Differentiation formulas

33 formulas and 78 common traps for MHT-CET Maths Differentiation, grouped by subtopic.

Full notes with worked examples

Foundations, the Chain Rule, and Differentiability

Learn this subtopic in the notes

Standard Derivatives and the Rules of Differentiation

Product rule

ddx[u(x) v(x)]=u′(x) v(x)+u(x) v′(x)\dfrac{d}{dx}\big[u(x)\,v(x)\big] = u'(x)\,v(x) + u(x)\,v'(x)
  • u,vu, vthe two factors being multiplied

The Chain Rule and Composite Functions

Chain rule

dydx=f′(g(x))⋅g′(x)for y=f(g(x))\dfrac{dy}{dx} = f'\big(g(x)\big) \cdot g'(x) \qquad \text{for } y = f(g(x))
  • ffouter function
  • g(x)g(x)inner function — its derivative is the multiplying factor

Differentiating Iterated Functions f(f(x))

Chain rule on an iterated function

ddxf(f(f(x)))=f′(f(f(x)))⋅f′(f(x))⋅f′(x)\dfrac{d}{dx}f\big(f(f(x))\big) = f'\big(f(f(x))\big)\cdot f'\big(f(x)\big)\cdot f'(x)

Simplify the Expression Before Differentiating

Quotient rule (used after simplifying)

ddx ⁣(uv)=u′v−uv′v2\dfrac{d}{dx}\!\left(\dfrac{u}{v}\right) = \dfrac{u'v - uv'}{v^2}

Linear Approximation Using the Derivative

Linear approximation

f(a+h)≈f(a)+h f′(a)f(a + h) \approx f(a) + h\,f'(a)
  • aanearby point with an easy exact value
  • hhsmall gap to the target (may be negative)

The Derivative as the Slope of the Tangent

Slope of the tangent

mtangent=dydx∣x=a=f′(a)m_{\text{tangent}} = \left.\dfrac{dy}{dx}\right|_{x=a} = f'(a)
  • f′(a)f'(a)instantaneous slope at x=ax = a

Differentiability and Where a Derivative Fails to Exist

Differentiability test

LHD=lim⁡h→0−f(a+h)−f(a)h=lim⁡h→0+f(a+h)−f(a)h=RHD\text{LHD} = \lim_{h\to0^-}\dfrac{f(a+h)-f(a)}{h} = \lim_{h\to0^+}\dfrac{f(a+h)-f(a)}{h} = \text{RHD}

Trigonometric Simplification Toolkit

The collapses you reach for most

1+cos⁡x=2cos⁡2x2,1−cos⁡x=2sin⁡2x2,1±sin⁡2x=∣sin⁡x±cos⁡x∣1+\cos x = 2\cos^2\tfrac{x}{2},\quad 1-\cos x = 2\sin^2\tfrac{x}{2},\quad \sqrt{1\pm\sin 2x}=|\sin x\pm\cos x|
  • x2\tfrac{x}{2}half-angle — appears whenever you collapse 1±cos⁡x1\pm\cos x
  • ∣⋯∣|\cdots|the root of a perfect square is a MODULUS; fix the sign on the given interval

Common traps

ddxax\dfrac{d}{dx}a^x is axlog⁡aa^x \log a, not x ax−1x\,a^{x-1}

Do not apply the power rule to a constant base. 2x2^x has a variable EXPONENT, so its derivative is 2xlog⁡22^x \log 2. The power rule nxn−1nx^{n-1} applies only to xnx^n (variable base, constant exponent). At x=0x = 0, ddx3x=log⁡3\dfrac{d}{dx}3^x = \log 3 — exactly the kind of value the bank tests.

Quotient rule sign: numerator is u′v−uv′u'v - uv'

The order matters — u′v−uv′u'v - uv', not uv′−u′vuv' - u'v. Writing it backwards flips the sign of the whole answer. Memorise it as 'low d-high minus high d-low, over low squared'.

Never forget the inner derivative factor

Differentiating sin⁡(3x2+1)\sin(3x^2+1) as just cos⁡(3x2+1)\cos(3x^2+1) drops the ×6x\times 6x — the single most common chain-rule error. Every layer contributes a multiplying factor.

Evaluate the inner argument, not the outer, when a factor is zero

For y=cos⁡(sin⁡x2)y = \cos(\sin x^2), dydx=−sin⁡(sin⁡x2)⋅cos⁡x2⋅2x\dfrac{dy}{dx} = -\sin(\sin x^2)\cdot \cos x^2 \cdot 2x. At x=π/2x = \sqrt{\pi/2}, x2=π/2x^2 = \pi/2 so cos⁡x2=0\cos x^2 = 0 — the whole product is 00. Spot the vanishing middle factor before grinding the arithmetic.

Drop the inner coefficient and you lose a factor

For g(x)=[f(2f(x)+2)]2g(x) = [f(2f(x) + 2)]^2 the chain rule contributes ×2\times 2 from the inner 2f(x)2f(x). Students who differentiate f(2f(x)+2)f(2f(x)+2) as if the inner were just f(x)f(x) miss this factor and get half the answer.

Don't try to find a formula for ff

These questions give only ff and f′f' at a point. You never need an explicit rule for ff — evaluate each chain-rule factor at the appropriate point and multiply. For f(f(f(x)))+(f(x))2f(f(f(x))) + (f(x))^2 at x=1x=1 with f(1)=1,f′(1)=3f(1)=1, f'(1)=3: 3⋅3⋅3+2⋅1⋅3=333\cdot3\cdot3 + 2\cdot1\cdot3 = 33.

Simplify first, or the algebra buries you

Differentiating x2/3−x−1/3x2/3+x−1/3\dfrac{x^{2/3} - x^{-1/3}}{x^{2/3} + x^{-1/3}} directly with the quotient rule is error-prone. Multiply through by x1/3x^{1/3} to get x−1x+1\dfrac{x-1}{x+1} — then y′=2(x+1)2y' = \dfrac{2}{(x+1)^2} and (x+1)2y′=2(x+1)^2 y' = 2 falls out instantly.

Pick hh small and signed correctly

To estimate log⁡10998\log_{10} 998, use a=1000a = 1000 and h=−2h = -2 (negative, since 998<1000998 < 1000). Getting the sign of hh wrong pushes the estimate the wrong way. With f′(x)=0.4343xf'(x) = \dfrac{0.4343}{x}: log⁡10998≈3−2⋅0.43431000=2.99913\log_{10} 998 \approx 3 - 2\cdot\dfrac{0.4343}{1000} = 2.99913.

The slope is the DERIVATIVE at aa, not at the target

Evaluate f′(a)f'(a) at the easy anchor point aa, not at a+ha + h. Using f′(a+h)f'(a+h) defeats the purpose — you wanted an easy slope.

Minimum SLOPE means differentiate twice

When a question asks where the slope (not the function) is minimum, you must differentiate again. First derivative f′(x)f'(x) IS the slope; set its derivative f′′(x)=0f''(x) = 0. Confusing 'minimum of yy' with 'minimum of y′y'' is a classic MHT-CET trap.

Simplify the curve before differentiating

2sin⁡θcos⁡θ=sin⁡2θ2\sin\theta\cos\theta = \sin 2\theta: the curve y=2exsin⁡(π4−x2)cos⁡(π4−x2)y = 2e^x \sin(\tfrac{\pi}{4} - \tfrac{x}{2})\cos(\tfrac{\pi}{4} - \tfrac{x}{2}) collapses to y=excos⁡xy = e^x \cos x before you ever differentiate. Spot the double-angle identity first.

Not every modulus is a non-differentiable point

Students reflexively answer 'fails at the corner' whenever they see ∣⋅∣|\cdot|. But f(x)=x1+∣x∣f(x) = \dfrac{x}{1 + |x|} is differentiable on ALL of R\mathbb{R}: the LHD and RHD at x=0x = 0 both equal 11. Always test LHD vs RHD at the suspect point — a vanishing or matching factor can smooth the corner, sometimes making the 'set of failure points' EMPTY.

Continuous does not mean differentiable

∣x∣|x| is continuous everywhere but has no derivative at 00. Differentiability is the stronger condition: differentiable ⇒\Rightarrow continuous, never the reverse.

1±cos⁡x1\pm\cos x (half-angle) vs 1±cos⁡2x1\pm\cos 2x (power-reduction)

Different collapses: 1−cos⁡x=2sin⁡2x21-\cos x = 2\sin^2\tfrac{x}{2} but 1−cos⁡2x=2sin⁡2x1-\cos 2x = 2\sin^2 x. Read the angle inside the cosine before choosing the factor — the wrong one halves or doubles the argument.

The root of a perfect square is a MODULUS

(sin⁡x−cos⁡x)2=∣sin⁡x−cos⁡x∣\sqrt{(\sin x-\cos x)^2} = |\sin x-\cos x|, not sin⁡x−cos⁡x\sin x-\cos x. Resolve the sign on the given interval: on (π4,π2)(\tfrac\pi4,\tfrac\pi2) it is +(sin⁡x−cos⁡x)+(\sin x-\cos x); on (0,π4)(0,\tfrac\pi4) it is −(sin⁡x−cos⁡x)-(\sin x-\cos x). Dropping the modulus flips the sign of the whole derivative.

sec⁡±tan⁡\sec\pm\tan — mind which way the half-angle shifts

sec⁡x+tan⁡x=tan⁡ ⁣(π4+x2)\sec x+\tan x=\tan\!\left(\tfrac\pi4+\tfrac x2\right) but sec⁡x−tan⁡x=tan⁡ ⁣(π4−x2)\sec x-\tan x=\tan\!\left(\tfrac\pi4-\tfrac x2\right). Useful check: (sec⁡x+tan⁡x)(sec⁡x−tan⁡x)=sec⁡2x−tan⁡2x=1(\sec x+\tan x)(\sec x-\tan x)=\sec^2x-\tan^2x=1.

Logarithmic Differentiation — Logs, Powers, and Long Products

Learn this subtopic in the notes

Logarithmic Differentiation — the Method

Derivative of f(x) raised to g(x)

ddx[f(x)g(x)]=f(x)g(x)[g′(x) log⁡f(x)+g(x) f′(x)f(x)]\frac{d}{dx}\left[f(x)^{g(x)}\right] = f(x)^{g(x)}\left[g'(x)\,\log f(x) + g(x)\,\frac{f'(x)}{f(x)}\right]
  • g′(x) log⁡f(x)g'(x)\,\log f(x)the term from differentiating the exponent (treat base as constant)
  • g(x) f′(x)/f(x)g(x)\,f'(x)/f(x)the term from differentiating the base (treat exponent as constant)

Products, Quotients and Powers via Logs

Log of a power-product

log⁡ ⁣(ap bqcr)=plog⁡a+qlog⁡b−rlog⁡c\log\!\left(\frac{a^{p}\,b^{q}}{c^{r}}\right) = p\log a + q\log b - r\log c

The Product Chain [(x+1)(2x+1)⋯(nx+1)] Evaluated at x=0

Power sums (the leftover at x=0)

∑k=1nk=n(n+1)2∑k=1nk2=n(n+1)(2n+1)6\sum_{k=1}^{n} k = \frac{n(n+1)}{2} \qquad \sum_{k=1}^{n} k^2 = \frac{n(n+1)(2n+1)}{6}
  • ppthe outer power (e.g. 22, 44, 3/23/2, or nn) — it just multiplies the sum
  • kkthe coefficient of xx in the kk-th factor; squared factors give ∑k2\sum k^2

Change of Base and log-of-a-log Forms

Change of base

log⁡ab=log⁡blog⁡a\log_a b = \frac{\log b}{\log a}
  • log⁡\lognatural log (base ee) throughout this chapter
  • aathe base — when it depends on xx, this is why you must convert

Square-Root Quotients with Inverse-Trig Arguments

Log of a square-root quotient

log⁡1−u1+u=12[log⁡(1−u)−log⁡(1+u)]\log\sqrt{\frac{1-u}{1+u}} = \frac{1}{2}\Big[\log(1-u) - \log(1+u)\Big]
  • uuthe inner function, e.g. sin⁡−1x\sin^{-1}x, with u′=1/1−x2u' = 1/\sqrt{1-x^2}
  • 1/21/2the coefficient produced by the outer square root

Common traps

Both terms appear — never use just one

For fgf^g, the "power rule" alone (gfg−1f′g f^{g-1}f') and the "exponential rule" alone (fglog⁡f⋅g′f^g\log f\cdot g') are each HALF the answer. Logarithmic differentiation produces BOTH terms and adds them. Using only one is the single most common error here.

A variable in the exponent kills the power rule

ddx(xx)\dfrac{d}{dx}(x^x) is NOT x⋅xx−1x\cdot x^{x-1}. The power rule ddxxn=nxn−1\dfrac{d}{dx}x^n = nx^{n-1} requires nn to be CONSTANT. When the exponent itself depends on xx, take logs.

cos⁻¹(sin θ) collapses before you differentiate

In mixed stems like cos⁡−1(sin⁡θ)+xx\cos^{-1}(\sin\theta) + x^x, use cos⁡−1(sin⁡θ)=π2−θ\cos^{-1}(\sin\theta) = \tfrac{\pi}{2} - \theta (for θ∈[0,π2]\theta\in[0,\tfrac{\pi}{2}]) to flatten the inverse-trig piece to a simple −θ′-\theta'; only the xxx^x part needs log differentiation. Mixing the two methods up wastes time.

If y is already a log, there is no 1/y

For y=log⁡(expression)y = \log(\text{expression}), expand the inside with log laws and differentiate the SUM directly. The 1ydydx\dfrac{1}{y}\dfrac{dy}{dx} form is only for log⁡y=⋯\log y = \cdots (i.e. you took the log yourself).

Simplify before you differentiate — log⁡1+sin⁡x1−sin⁡x\log\sqrt{\frac{1+\sin x}{1-\sin x}}

Some quotient-log stems collapse to a tidy single function. log⁡1+sin⁡x1−sin⁡x=log⁡tan⁡ ⁣(π4+x2)\log\sqrt{\tfrac{1+\sin x}{1-\sin x}} = \log\tan\!\left(\tfrac{\pi}{4}+\tfrac{x}{2}\right), whose derivative is the clean sec⁡x\sec x. Charging in with the quotient rule on the raw fraction works but is far slower and error-prone.

A fractional exponent becomes a fractional COEFFICIENT

log⁡[(x+5)4/3]=43log⁡(x+5)\log[(x+5)^{4/3}] = \tfrac{4}{3}\log(x+5), not 43(x+5)\tfrac{4}{3}(x+5) and not (x+5)4/3log⁡(x+5)^{4/3}\log. Drop the exponent out front; do not leave it on the argument.

Substitute x=0 only AFTER differentiating

If you plug x=0x=0 into yy before differentiating, you get the constant 11 and derivative 00 — wrong. Differentiate the log-sum fully (keep xx), THEN set x=0x=0 so the denominators collapse to 11.

Squared factor ⇒\Rightarrow ∑k2\sum k^2, not ∑k\sum k

If the kk-th factor is k2x+1k^2x+1 (i.e. 1,4x+1,9x+1,…1, 4x+1, 9x+1,\ldots), differentiating log⁡(k2x+1)\log(k^2x+1) gives k2k2x+1\dfrac{k^2}{k^2x+1}, so the leftover sum is ∑k2=n(n+1)(2n+1)6\sum k^2 = \tfrac{n(n+1)(2n+1)}{6}. Don't reflexively write ∑k\sum k.

Product like (1-x)(2-x)⋯(n-x) at x=1 — factor, don't sum

When a factor itself VANISHES at the evaluation point (here (1−x)=0(1-x)=0 at x=1x=1), the 1yy′\dfrac{1}{y}y' form blows up. Instead write y=(1−x) g(x)y=(1-x)\,g(x); then y′(1)=−1⋅g(1)y'(1) = -1\cdot g(1), where g(1)g(1) is the product of the remaining factors at x=1x=1.

The outer power just multiplies the sum

A power 3/23/2 or nn on the whole product becomes a coefficient pp in log⁡y=p∑log⁡(⋯ )\log y = p\sum\log(\cdots). So the answer is always p∑kp\sum k (or p∑k2p\sum k^2) — e.g. power 3/23/2 gives 32⋅n(n+1)2=3n(n+1)4\tfrac{3}{2}\cdot\tfrac{n(n+1)}{2} = \tfrac{3n(n+1)}{4}.

Convert the variable base BEFORE differentiating

ddxlog⁡sin⁡x(tan⁡x)\dfrac{d}{dx}\log_{\sin x}(\tan x) cannot be done with the 1u\dfrac{1}{u} rule directly — the base sin⁡x\sin x is not constant. Always rewrite as log⁡tan⁡xlog⁡sin⁡x\dfrac{\log\tan x}{\log\sin x} first, then use the quotient rule.

A vanishing log term kills half the quotient rule

At nice points (x=π/4x=\pi/4 gives log⁡tan⁡x=0\log\tan x = 0; x=ex=e gives log⁡log⁡x=0\log\log x = 0), the quotient-rule term multiplying that zero disappears. Spot the vanishing term FIRST — it saves most of the algebra. The bank answer for log⁡sin⁡xtan⁡x\log_{\sin x}\tan x at π/4\pi/4 is −4log⁡2-4\log 2.

log of a log is NOT (log)²

log⁡(log⁡x)\log(\log x) is a composition (log applied to log⁡x\log x), with derivative 1log⁡x⋅1x\dfrac{1}{\log x}\cdot\dfrac{1}{x}. It is not (log⁡x)2(\log x)^2, whose derivative would be 2log⁡x⋅1x2\log x\cdot\tfrac{1}{x}. Keep the two straight.

Don't forget the chain factor u' on the inverse-trig inner

When u=sin⁡−1xu = \sin^{-1}x, each log⁡(1±u)\log(1\pm u) differentiates to ±u′1±u\dfrac{\pm u'}{1\pm u} with u′=11−x2u' = \dfrac{1}{\sqrt{1-x^2}}. Dropping the u′u' (treating uu as xx) is a frequent error; at x=0x=0 it happens to equal 11, but you must include it in general.

Compute y at the point — usually y=1 at x=0

You multiply 1yy′\dfrac{1}{y}y' by yy to finish. At x=0x=0 the quotient under the root is 11=1\tfrac{1}{1}=1, so y=1y=1 and the multiply-back is trivial. Forgetting to put yy back (leaving only 1yy′\tfrac{1}{y}y') gives the wrong magnitude when y≠1y\neq 1.

Watch which factor is on top — it sets the sign

1−sin⁡−1x1+sin⁡−1x\sqrt{\tfrac{1-\sin^{-1}x}{1+\sin^{-1}x}} gives −1-1 at x=0x=0; flipping to 1+sin⁡−1x1−sin⁡−1x\sqrt{\tfrac{1+\sin^{-1}x}{1-\sin^{-1}x}} gives +1+1. The numerator/denominator order flips every sign — read the stem carefully before reaching for a memorised answer.

Implicit Differentiation and Special Forms

Learn this subtopic in the notes

Implicit Differentiation — the Core Method

Implicit chain rule

ddx[g(y)]=g′(y) dydx,ddx(xy)=y+xdydx\frac{d}{dx}\big[g(y)\big] = g'(y)\,\frac{dy}{dx}, \qquad \frac{d}{dx}(xy)=y+x\frac{dy}{dx}
  • dydx\frac{dy}{dx}the unknown you collect and solve for
  • g(y)g(y)any function of yy; its xx-derivative carries dydx\frac{dy}{dx}

Implicit Relations like log(x + y) = 2xy

Differentiating log(x + y)

ddxlog⁡(x+y)=1x+y(1+dydx)\frac{d}{dx}\log(x+y) = \frac{1}{x+y}\left(1 + \frac{dy}{dx}\right)
  • 1+dydx1 + \frac{dy}{dx}the chain-rule derivative of the inner x+yx+y

Exponential Relations — Take Logs, Then Differentiate

Log first, then differentiate

ddx[u(x) log⁡v(x)]=u′log⁡v+u⋅v′v\frac{d}{dx}\big[u(x)\,\log v(x)\big] = u'\log v + u\cdot\frac{v'}{v}
  • u(x)u(x)the exponent (often containing yy)
  • log⁡v(x)\log v(x)log of the base, after taking logs of both sides

Relations of the Form tan y = (rational in x)

Standard result

tan⁡y=xsin⁡α1−xcos⁡α  ⇒  dydx=sin⁡α1−2xcos⁡α+x2\tan y = \frac{x\sin\alpha}{1 - x\cos\alpha} \;\Rightarrow\; \frac{dy}{dx} = \frac{\sin\alpha}{1 - 2x\cos\alpha + x^2}
  • sec⁡2y\sec^2 yrewritten as 1+tan⁡2y1 + \tan^2 y to substitute the given expression

Proving a Given Differential Relation

Key explicit form

y1/m+y−1/m=2x  ⇒  y=(x+x2−1)my^{1/m} + y^{-1/m} = 2x \;\Rightarrow\; y = \left(x + \sqrt{x^2-1}\right)^{m}
  • t=y1/mt = y^{1/m}substitution that turns the relation into a quadratic in tt

Self-Referential Infinite Expressions

Self-reference for a nested radical

y=f(x)+y  ⇒  y2=f(x)+y  ⇒  dydx=f′(x)2y−1y = \sqrt{f(x) + y} \;\Rightarrow\; y^2 = f(x) + y \;\Rightarrow\; \frac{dy}{dx} = \frac{f'(x)}{2y - 1}
  • yythe whole infinite expression — it reappears under the first root

Functional Equations — Find f, Then Differentiate

Reciprocal-substitution setup

af(x)+bf ⁣(1x)=g(x),then x→1x:  af ⁣(1x)+bf(x)=g ⁣(1x)a f(x) + b f\!\left(\tfrac{1}{x}\right) = g(x), \quad\text{then } x\to\tfrac1x:\; a f\!\left(\tfrac1x\right) + b f(x) = g\!\left(\tfrac1x\right)
  • f′(1),f′′(2)f'(1), f''(2)treat as unknown CONSTANTS, solve via coefficient comparison

Common traps

Differentiating a y-term without the dy/dx factor

ddx(y2)\dfrac{d}{dx}(y^2) is 2ydydx2y\dfrac{dy}{dx}, NOT 2y2y. The whole method rests on attaching dydx\dfrac{dy}{dx} to every yy-derivative by the chain rule. Drop it and every answer is wrong.

Forgetting the product rule on the xy term

ddx(xy)=y+xdydx\dfrac{d}{dx}(xy) = y + x\dfrac{dy}{dx} — it has TWO terms because both factors carry an xx-dependence. Writing just xdydxx\dfrac{dy}{dx} or just yy loses half the term.

Find the y-value before substituting into the derivative

The derivative formula contains both xx and yy. At x=0x=0 you still need yy; get it from the ORIGINAL equation (e.g. log⁡y=0⇒y=1\log y = 0 \Rightarrow y=1) before plugging into y′y'. Substituting only x=0x=0 leaves the answer undetermined.

log(x + y) = sin(x + y) collapses to slope -1

When both sides are functions of the single quantity x+yx+y, differentiating factors out (1+y′)(1+y'). Setting it to zero gives y′=−1y' = -1, independent of the functions — recognise this shortcut for log⁡(x+y)=sin⁡(x+y)\log(x+y)=\sin(x+y) and its cousins.

You cannot use the power rule when the exponent contains y

ddx(xy)\dfrac{d}{dx}(x^{y}) is NOT yxy−1yx^{y-1} — that rule needs a CONSTANT power. Because yy varies, take logs first: log⁡(xy)=ylog⁡x\log(x^{y}) = y\log x, then differentiate the product.

Use the original (logged) relation to simplify the final answer

These answers are meant to come out clean. After collecting y′y', substitute yy from the logged equation (e.g. y=x/(1+log⁡x)y = x/(1+\log x)) — that is what turns a messy fraction into the tidy form the options expect.

Differentiate tan y as sec-squared y times dy/dx

ddx(tan⁡y)=sec⁡2y dydx\dfrac{d}{dx}(\tan y) = \sec^2 y\,\dfrac{dy}{dx} — the dydx\dfrac{dy}{dx} is essential (chain rule on the implicit yy). Then convert sec⁡2y\sec^2 y to 1+tan⁡2y1+\tan^2 y so the given relation can be substituted.

Spotting a hidden inverse-tangent shortcut

If the rational in xx is exactly 2x1−x2\dfrac{2x}{1-x^2} (or x+a1−ax\dfrac{x+a}{1-ax}), it is a tan⁡\tan addition/double-angle in disguise. Recognising it lets you write yy explicitly and skip the heavy quotient differentiation.

Use the substitution to get y explicitly first

Trying to differentiate y1/m+y−1/m=2xy^{1/m}+y^{-1/m}=2x directly is painful. Set t=y1/mt=y^{1/m}, solve the resulting quadratic for yy, THEN differentiate — the proof falls out in two lines.

Square only after isolating the root

The target identities carry a (x2−1)(x^2-1) or (x2+1)(x^2+1) factor because y′y' has a x2±1\sqrt{x^2\pm1} in its denominator. Square y′y' to clear that root — squaring is what produces the polynomial coefficient.

The inner expression equals the WHOLE y, not part of it

Because the nesting is infinite, what sits under the first root is f(x)+(the same infinite expression)=f(x)+yf(x) + (\text{the same infinite expression}) = f(x) + y. Treating it as a finite tower (or as just f(x)f(x)) breaks the self-reference that makes the problem solvable.

Square before differentiating, not after

Convert y=f(x)+yy = \sqrt{f(x)+y} into y2=f(x)+yy^2 = f(x)+y FIRST, then differentiate. Differentiating the square root directly forces a chain-rule mess; the squared form differentiates in one clean line.

f'(1), f''(2) are CONSTANTS — name them and solve

In f(x)=x3+x2f′(1)+xf′′(2)+6f(x)=x^3+x^2f'(1)+xf''(2)+6, the terms f′(1)f'(1) and f′′(2)f''(2) are fixed numbers, not functions. Let them be a,ba, b, build f′f' and f′′f'', evaluate at the stated points, and solve the resulting linear system.

For f(x) and f(1/x), substitute x to 1/x to get a second equation

One equation in two unknowns f(x)f(x) and f(1/x)f(1/x) is not enough. Replacing xx by 1/x1/x gives an independent equation; solve the pair simultaneously to isolate f(x)f(x) before differentiating.

f'(x) = f(x) means exponential

The only functions satisfying f′=ff'=f are f(x)=Cexf(x)=Ce^{x}. Use the given value (e.g. f(1)=2f(1)=2) to fix CC, then differentiate compositions like h(x)=f(f(x))h(x)=f(f(x)) by the chain rule.

Inverse Functions and Inverse Trigonometric Differentiation

Learn this subtopic in the notes

Derivative of an inverse function

g′(x)=1f′(g(x))where g=f−1g'(x) = \dfrac{1}{f'\big(g(x)\big)} \qquad\text{where } g = f^{-1}
  • g(x)g(x)the inverse f−1(x)f^{-1}(x) — the input that maps to xx under ff
  • f′(g(x))f'(g(x))slope of ff at the matching point, NOT f′(x)f'(x)

The Inverse Trigonometric Derivative Table

Chain rule on an inverse-trig function

ddxtan⁡−1(u)=11+u2⋅dudx\dfrac{d}{dx}\tan^{-1}(u) = \dfrac{1}{1+u^2}\cdot\dfrac{du}{dx}
  • uuthe inner function (e.g. x2x^2, 3x3x, log⁡x\log x)
  • du/dxdu/dxderivative of the inner function — never forget it

Collapsing Inverse-Trig with a Substitution

The two workhorse collapses

sin⁡−1 ⁣(3x−4x3)=3sin⁡−1x,tan⁡−1 ⁣2x1−x2=2tan⁡−1x\sin^{-1}\!\big(3x - 4x^3\big) = 3\sin^{-1}x, \qquad \tan^{-1}\!\dfrac{2x}{1-x^2} = 2\tan^{-1}x
  • x=sin⁡θx = \sin\thetause when the argument is a sine multiple-angle (3x−4x33x-4x^3, 2x1−x22x\sqrt{1-x^2})
  • x=tan⁡θx = \tan\thetause when the argument is a tangent/double-angle ratio

tan inverse Addition and Complementary Identities

Arctan addition + complementary pair

tan⁡−1x+tan⁡−1y=tan⁡−1 ⁣x+y1−xy,sin⁡−1x+cos⁡−1x=π2\tan^{-1}x + \tan^{-1}y = \tan^{-1}\!\dfrac{x+y}{1-xy}, \qquad \sin^{-1}x + \cos^{-1}x = \dfrac{\pi}{2}
  • 1−xy1 - xydenominator of the combined argument; sign flips for the subtraction form
  • π/2\pi/2the constant a complementary pair collapses to — derivative 00

Differentiating One Inverse-Trig with Respect to Another

Ratio of angle-multiples

If u=a θ and v=b θ, then dudv=ab\text{If } u = a\,\theta \text{ and } v = b\,\theta, \text{ then } \dfrac{du}{dv} = \dfrac{a}{b}
  • a,ba, bthe constant multiples after each function collapses to a multiple of θ\theta
  • dθd\thetacancels in the ratio — never appears in the final answer

Exponentials of Inverse-Trig Functions

Logarithmic-derivative ratio

h(x)=eg(x)  ⇒  h′(x)h(x)=g′(x)h(x) = e^{g(x)} \;\Rightarrow\; \dfrac{h'(x)}{h(x)} = g'(x)
  • g(x)g(x)the inner inverse-trig exponent (e.g. sin⁡−1x\sin^{-1}x)
  • h′/hh'/hthe exponential cancels, leaving just g′(x)g'(x)

Common traps

Evaluate f′f' at g(x)g(x), never at xx

The single most common error: writing g′(x)=1/f′(x)g'(x) = 1/f'(x). It is g′(x)=1/f′(g(x))g'(x) = 1/f'(g(x)). At a numeric point you must first find g(a)g(a) (the input mapping to aa), then plug THAT into f′f'.

You rarely need the formula for f−1f^{-1}

For a point value, don't invert ff algebraically — just find the matching input bb with f(b)=af(b) = a and take 1/f′(b)1/f'(b). Inverting an awkward cubic-plus-exponential is impossible anyway; the reciprocal rule sidesteps it.

Don't forget the inner derivative du/dxdu/dx

ddxsin⁡−1(3x)\dfrac{d}{dx}\sin^{-1}(3x) is NOT 11−9x2\dfrac{1}{\sqrt{1-9x^2}} — you must multiply by the inner derivative 33. The chain factor is what most option-traps omit.

The minus sign rides on the 'co' functions

cos⁡−1\cos^{-1}, cot⁡−1\cot^{-1}, cosec⁡−1\operatorname{cosec}^{-1} carry the negative sign; their partners sin⁡−1\sin^{-1}, tan⁡−1\tan^{-1}, sec⁡−1\sec^{-1} are positive. Mixing the sign flips the answer onto a distractor.

sec⁡\sec and cosec⁡\operatorname{cosec} derivatives carry ∣x∣|x|

ddxsec⁡−1x=1∣x∣x2−1\dfrac{d}{dx}\sec^{-1}x = \dfrac{1}{|x|\sqrt{x^2-1}} — the absolute value on xx is part of the formula. Dropping it is a quiet error the bank tests.

Match the substitution to the argument's shape

3x−4x33x-4x^3 screams x=sin⁡θx=\sin\theta (it is sin⁡3θ\sin 3\theta); 4x3−3x4x^3-3x screams x=cos⁡θx=\cos\theta (it is cos⁡3θ\cos 3\theta); ratios with 1+x21+x^2/1−x21-x^2 scream x=tan⁡θx=\tan\theta. Picking the wrong one buries the simplification.

Watch the principal-value branch

sin⁡−1(sin⁡α)=α\sin^{-1}(\sin\alpha) = \alpha only inside [−π/2,π/2][-\pi/2,\pi/2]. When the substituted angle leaves that range — e.g. at x=12x=\tfrac12 in sin⁡−1 ⁣2⋅3x1+9x\sin^{-1}\!\frac{2\cdot 3^x}{1+9^x}, where 2θ=2π/3>π/22\theta = 2\pi/3 > \pi/2 — the collapse becomes π−\pi - (angle), flipping the sign of the derivative.

Exponential/log inner functions hide the same shapes

2log⁡x1+(log⁡x)2\dfrac{2\log x}{1+(\log x)^2} is sin⁡2ϕ\sin 2\phi with log⁡x=tan⁡ϕ\log x = \tan\phi, collapsing to 2tan⁡−1(log⁡x)2\tan^{-1}(\log x). Substitute on the INNER expression (log⁡x\log x, 3x3^x), then chain the extra inner derivative when differentiating.

The constant differentiates to zero — but only if you SEE it

A sum of arctans that collapses to a constant has derivative 00. Students grind out two quotient-rule derivatives and miss that the whole thing was π/4+\pi/4 + constant. Always test for the addition/complementary pattern first.

Mind the 1∓xy1 \mp xy sign and the validity range

Addition uses 1−xy1-xy in the denominator, subtraction uses 1+xy1+xy. The split tan⁡−1x+y1−xy=tan⁡−1x+tan⁡−1y\tan^{-1}\frac{x+y}{1-xy} = \tan^{-1}x + \tan^{-1}y is exact only when xy<1xy < 1; outside that a ±π\pm\pi correction appears (a constant, so the derivative is unchanged — but the function value differs).

Don't differentiate w.r.t. xx separately and then divide blindly

You CAN compute du/dxdv/dx\dfrac{du/dx}{dv/dx}, but the elegant route is to collapse both to multiples of one angle and take the ratio. The shortcut avoids messy 1−x2\sqrt{1-x^2} factors that cancel anyway.

Both functions must share ONE angle

If one collapses with x=sin⁡θx=\sin\theta and the other with x=cos⁡ϕx=\cos\phi, convert via cos⁡−1x=π2−sin⁡−1x\cos^{-1}x = \frac{\pi}{2}-\sin^{-1}x so both are in the same θ\theta. Mixing two different angle variables corrupts the ratio (and can flip the sign).

h′/hh'/h strips the exponential — don't carry it

Because h′(x)=h(x) g′(x)h'(x) = h(x)\,g'(x), the ratio h′/hh'/h is just g′(x)g'(x) with no e(⋯ )e^{(\cdots)} left. Distractors keep the exponential in the answer; the clean ratio doesn't.

The sign comes from the inner inverse-trig

esin⁡−1xe^{\sin^{-1}x} gives +11−x2+\frac{1}{\sqrt{1-x^2}}; ecos⁡−1xe^{\cos^{-1}x} gives −11−x2-\frac{1}{\sqrt{1-x^2}}. The exponential is always positive, so the sign is decided entirely by g′(x)g'(x).

For monotonicity, check the SIGN of g′g', not its messiness

g′(u)=2eu1+e2ug'(u) = \frac{2e^u}{1+e^{2u}} looks complicated, but eu>0e^u>0 and the denominator >0>0, so g′>0g'>0 everywhere — strictly increasing. You don't need to simplify further to conclude monotonicity.

Parametric Differentiation, Second Derivatives & Proving Relations

Learn this subtopic in the notes

Parametric Differentiation

Parametric first derivative

dydx= dy/dt  dx/dt ,dxdt≠0\dfrac{dy}{dx} = \dfrac{\,dy/dt\,}{\,dx/dt\,}, \qquad \dfrac{dx}{dt} \neq 0
  • ttthe parameter (often θ\theta) linking xx and yy
  • dx/dt≠0dx/dt \neq 0needed so the slope is defined

Second Derivative of a Parametric Function

Parametric second derivative

d2ydx2=ddt ⁣(dydx)dxdt\dfrac{d^2y}{dx^2} = \dfrac{\dfrac{d}{dt}\!\left(\dfrac{dy}{dx}\right)}{\dfrac{dx}{dt}}
  • d/dt(dy/dx)d/dt(dy/dx)differentiate the first slope (a function of tt) again w.r.t. tt
  • dx/dtdx/dtdivide by it once more — the chain-rule leftover

Proving Second-Order Relations

Two standard second-order relations

y=Acos⁡nx+Bsin⁡nx⇒y′′=−n2y;y=axn+1+bx−n⇒x2y′′=n(n+1)yy = A\cos nx + B\sin nx \Rightarrow y'' = -n^2 y; \qquad y = ax^{n+1} + bx^{-n} \Rightarrow x^2 y'' = n(n+1)y
  • y′′=−n2yy'' = -n^2 ythe SHM-type relation from the sin/cos combination
  • n(n+1)yn(n+1)ythe multiple that appears for the power combination

Showing an Expression Is Constant

Zero derivative implies constant

ddxE(x)=0 for all x ⟹ E(x)=const,E(b)=E(a)\dfrac{d}{dx}E(x) = 0 \ \text{for all } x \ \Longrightarrow\ E(x) = \text{const}, \quad E(b) = E(a)

nth-Order Derivatives — Standard Results

nth derivative of a sine with linear argument

dndxn(sin⁡(ax+b))=ansin⁡ ⁣(ax+b+nπ2)\dfrac{d^n}{dx^n}\big(\sin(ax+b)\big) = a^n \sin\!\left(ax+b+\dfrac{n\pi}{2}\right)
  • ana^nthe coefficient aa factors out once per differentiation
  • nπ/2n\pi/2each derivative advances the phase by a quarter-turn

Common traps

Do not flip the ratio

The slope is dy/dtdx/dt\dfrac{dy/dt}{dx/dt} — the parameter-derivative of yy on top, of xx on the bottom. Writing dx/dtdy/dt\dfrac{dx/dt}{dy/dt} gives the reciprocal slope and a wrong answer.

The slope can stay in terms of the parameter

There is no rule that says dydx\dfrac{dy}{dx} must be a function of xx. Leaving it as 1t\dfrac{1}{t} or −bacot⁡θ-\dfrac{b}{a}\cot\theta is the final form; only substitute a parameter value when the question asks for the slope at a point.

NEVER divide the two second derivatives

d2ydx2≠d2y/dt2d2x/dt2\dfrac{d^2y}{dx^2} \neq \dfrac{d^2y/dt^2}{d^2x/dt^2}. This is the single most common parametric error in MHT-CET. The correct route is: find dy/dxdy/dx, differentiate it with respect to the parameter, then divide by dx/dtdx/dt.

Differentiate dy/dx with respect to t, not x

After you have dydx\dfrac{dy}{dx} as a function of tt, you cannot differentiate it directly with respect to xx. Differentiate it with respect to tt and then divide by dxdt\dfrac{dx}{dt} to convert back to a derivative in xx.

Carry the constants — they cancel cleanly

In y=Acos⁡nx+Bsin⁡nxy = A\cos nx + B\sin nx, differentiating twice brings down −n2-n^2 from BOTH terms identically, so the whole bracket reforms into yy. Do not drop AA or BB — the relation only emerges because both terms behave the same way.

Match the power-combination exponents

For y=axn+1+bx−ny = ax^{n+1} + bx^{-n} the relation x2y′′=n(n+1)yx^2 y'' = n(n+1)y holds only because both exponents are tuned to give the SAME factor n(n+1)n(n+1) after two derivatives. If the exponents are arbitrary, no single relation appears — read them carefully.

Zero derivative means constant — the second point is a decoy

Once E′(x)=0E'(x) = 0, the specific points (5 and 10, say) carry no information beyond the given value. E(10)=E(5)E(10) = E(5) exactly. Students waste time trying to compute EE at the new point from scratch.

Use the supplied relations during differentiation

Expressions like (f)2+(g)2(f)^2 + (g)^2 only collapse to zero because of the given conditions f′′=−ff'' = -f and g=f′g = f'. Substitute them as soon as g′g' or f′′f'' appears — that substitution is exactly what produces the cancellation.

Sine and cosine cycle with period 4 in the order n

Differentiating sin⁡x\sin x four times returns to sin⁡x\sin x; the nπ2\tfrac{n\pi}{2} phase term encodes exactly this 4-step cycle. Reduce nn modulo 4 if you prefer to evaluate the phase directly.

The power-rule nth derivative stops at zero

dndxn(xm)=m!(m−n)!xm−n\dfrac{d^n}{dx^n}(x^m) = \dfrac{m!}{(m-n)!}x^{m-n} is valid only for m≥nm \geq n. Once n>mn > m every further derivative of a polynomial term is 00 — the factorial pattern would otherwise give a meaningless negative factorial.

Differentiating One Function With Respect to Another

Learn this subtopic in the notes

Differentiating One Function With Respect to Another

Derivative of u with respect to v

dudv=dudxdvdx,dvdx≠0\dfrac{du}{dv} = \dfrac{\dfrac{du}{dx}}{\dfrac{dv}{dx}}, \qquad \dfrac{dv}{dx} \neq 0
  • u=f(x)u = f(x)the function being differentiated (the 'top')
  • v=g(x)v = g(x)the function we differentiate with respect to (the 'bottom')
  • dv/dx≠0dv/dx \neq 0ratio is undefined where the bottom's derivative vanishes

Composite Functions Using Given Derivatives f' and g'

Composite-over-composite ratio

d [f(p(x))]d [g(q(x))]=f′(p(x)) p′(x)g′(q(x)) q′(x)\dfrac{d\,[f(p(x))]}{d\,[g(q(x))]} = \dfrac{f'(p(x))\,p'(x)}{g'(q(x))\,q'(x)}
  • f′(p(x))f'(p(x))outer derivative of the top, read from the given f' value
  • p′(x)p'(x)inner derivative of the top function
  • g′(q(x))g'(q(x))outer derivative of the bottom, read from the given g' value
  • q′(x)q'(x)inner derivative of the bottom function

Common traps

Do NOT differentiate one function directly by the other

dudv\dfrac{du}{dv} is not 'differentiate uu and substitute vv'. You must form both dudx\dfrac{du}{dx} and dvdx\dfrac{dv}{dx} and divide. There is no shortcut that skips xx.

Substitute the point only after dividing

If a value like x=5x = 5 is given, keep xx symbolic while you form du/dxdv/dx\dfrac{du/dx}{dv/dx}, then substitute. Plugging the point into dudx\dfrac{du}{dx} and dvdx\dfrac{dv}{dx} before simplifying invites arithmetic slips.

The bottom's derivative must be non-zero

dudv=du/dxdv/dx\dfrac{du}{dv} = \dfrac{du/dx}{dv/dx} is only valid where dvdx≠0\dfrac{dv}{dx} \neq 0. If v=g(x)v = g(x) has a stationary point at the value asked, the rate of change with respect to vv is undefined there.

Each inner derivative must be carried through

When the top is f(sec⁡x)f(\sec x), its derivative is f′(sec⁡x)⋅sec⁡xtan⁡xf'(\sec x)\cdot\sec x\tan x — the inner sec⁡xtan⁡x\sec x\tan x is part of it. Forgetting the inner derivative is the most common slip and silently drops a factor.

Match each supplied value to the right inner argument

A given f′(2)f'(\sqrt{2}) is meant for where the inner function equals 2\sqrt{2} (e.g. sec⁡π4=2\sec\frac{\pi}{4} = \sqrt{2}) — not for x=2x = \sqrt{2}. Evaluate the inner function at the given xx first, then read off the matching f′f' value.

Keep the negative sign on falling inner functions

If the bottom is g(cos⁡x)g(\cos x), its inner derivative is −sin⁡x-\sin x; the minus sign stays in the denominator and sets the sign of the final answer. Drop it and you get the right magnitude with the wrong sign.

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