Limits and Derivatives

Every real change — a car speeding up, a chemical reaction proceeding, a falling stone gathering speed — poses the same question: how fast is something changing right now, at one instant, not on average over some stretch of time? Ordinary algebra tells you how far a body travels in five seconds; it has no word for "at this instant." This chapter builds that word, and it does so by chaining together two ideas that turn out to be the same idea seen twice: the limit and the derivative. We begin exactly as NCERT does, with a stone dropped from a cliff, s=4.9t2s = 4.9t^2 metres in tt seconds. Average velocity over any interval is easy — divide distance by time — but the average velocity from t=1.99t=1.99 to t=2t=2 is not the velocity at t=2t=2. To pin that down, the chapter shrinks the interval smaller and smaller and watches the average velocity settle toward a single number. That settling-down process is the seed of the idea of a limit: the value a function is heading toward as its input approaches a point, whether or not the function is even defined there. From this intuition the chapter builds a formal toolkit: the left hand limit and right hand limit, an algebra of limits that lets a complicated limit be broken into simpler pieces, a standard result for lim⁡x→axn−anx−a\lim_{x\to a}\frac{x^n-a^n}{x-a}, and — via a beautiful geometric squeeze called the sandwich theorem — the two limits that unlock every trigonometric derivative, lim⁡x→0sin⁡xx=1\lim_{x\to 0}\frac{\sin x}{x}=1 and lim⁡x→01−cos⁡xx=0\lim_{x\to 0}\frac{1-\cos x}{x}=0. With limits secured, the chapter defines the derivative f′(x)f'(x) as the limit of the slope of a secant line as it collapses onto a tangent, builds an algebra of derivatives (sum, product, quotient rules), and computes the derivatives of xnx^n, sin⁡x\sin x, cos⁡x\cos x and tan⁡x\tan x from first principles. By the end you should be able to evaluate any polynomial, rational or trigonometric limit that reduces to a 00\tfrac{0}{0} form, find a derivative from first principles, and apply the standard results fluently — exactly the toolkit Class 12 calculus, and JEE/NEET, will assume you already own.

Key takeaways
  • A limit lim⁡x→af(x)=l\lim_{x\to a} f(x) = l is the value f(x)f(x) is expected to take at x=ax=a, based on the values of ff near aa — it need not equal f(a)f(a), and f(a)f(a) need not even exist.
  • The left hand limit and right hand limit are the values dictated by points just below aa and just above aa respectively; the two-sided limit exists only when both agree.
  • The algebra of limits (Theorem 1) says that if lim⁡f(x)\lim f(x) and lim⁡g(x)\lim g(x) both exist at x=ax=a, then the limit of the sum, difference, product and quotient of ff and gg equal the sum, difference, product and quotient of the limits (quotient needs the denominator's limit to be non-zero).
  • The standard result lim⁡x→axn−anx−a=nan−1\lim_{x\to a}\dfrac{x^n-a^n}{x-a} = n a^{n-1} (Theorem 2) turns limits involving powers into pure algebra, and holds even for rational nn when a>0a>0.
  • For rational functions of the 00\tfrac{0}{0} form at x=ax=a, factor out and cancel (x−a)(x-a) — legitimate because the limiting process never actually sets xx equal to aa.
  • Two trigonometric limits, proved by a geometric squeeze (the sandwich theorem): lim⁡x→0sin⁡xx=1\lim_{x\to 0}\dfrac{\sin x}{x} = 1 and lim⁡x→01−cos⁡xx=0\lim_{x\to 0}\dfrac{1-\cos x}{x} = 0.
  • The derivative of ff at aa is f′(a)=lim⁡h→0f(a+h)−f(a)hf'(a) = \lim_{h\to 0}\dfrac{f(a+h)-f(a)}{h} — the first principle of differentiation — and geometrically it is the slope of the tangent to y=f(x)y=f(x) at x=ax=a.
  • The algebra of derivatives gives (f±g)′=f′±g′(f\pm g)' = f'\pm g', the Leibniz product rule (uv)′=u′v+uv′(uv)' = u'v+uv', and the quotient rule (uv)′=u′v−uv′v2\left(\dfrac{u}{v}\right)' = \dfrac{u'v-uv'}{v^2}.
  • Standard derivatives: ddx(xn)=nxn−1\dfrac{d}{dx}(x^n) = nx^{n-1}, ddx(sin⁡x)=cos⁡x\dfrac{d}{dx}(\sin x) = \cos x, ddx(cos⁡x)=−sin⁡x\dfrac{d}{dx}(\cos x) = -\sin x, and ddx(tan⁡x)=sec⁡2x\dfrac{d}{dx}(\tan x) = \sec^2 x.
  • Key idea: a limit is the value a function is heading toward as x approaches a point, and the derivative is exactly the limit of the average rate of change over a shrinking interval — the slope of a secant line collapsing onto the tangent.
The core insight

The derivative f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x) = \lim_{h\to 0}\dfrac{f(x+h)-f(x)}{h} is nothing but the limit of an average rate of change as the interval shrinks to zero, so the entire machinery of limits — left and right hand limits, the algebra of limits, the standard result lim⁡xn−anx−a=nan−1\lim\frac{x^n-a^n}{x-a}=na^{n-1}, and the sandwich-theorem limits lim⁡sin⁡xx=1\lim\frac{\sin x}{x}=1 and lim⁡1−cos⁡xx=0\lim\frac{1-\cos x}{x}=0 — feeds directly into an algebra of derivatives (sum, product, quotient rules) that computes the slope of the tangent to any curve.

What this chapter covers

The chapter opens with a physical motivation — the falling stone — that manufactures the idea of an instantaneous rate of change before any formal definition is given. It then formalises the limit: left hand and right hand limits, when a two-sided limit exists, and an algebra of limits (sum, difference, product, quotient) that turns limit-evaluation into ordinary algebra. Two standard results are proved and used relentlessly: lim⁡x→axn−anx−a=nan−1\lim_{x\to a}\frac{x^n-a^n}{x-a}=na^{n-1}, which handles every limit built from powers of xx, and the trigonometric pair lim⁡x→0sin⁡xx=1\lim_{x\to 0}\frac{\sin x}{x}=1, lim⁡x→01−cos⁡xx=0\lim_{x\to 0}\frac{1-\cos x}{x}=0, proved by squeezing sin⁡xx\frac{\sin x}{x} between cos⁡x\cos x and 11 (the sandwich theorem). The chapter then pivots to derivatives: f′(a)=lim⁡h→0f(a+h)−f(a)hf'(a)=\lim_{h\to 0}\frac{f(a+h)-f(a)}{h}, read geometrically as the slope of the tangent line, and generalised to the derivative function f′(x)f'(x). An algebra of derivatives mirrors the algebra of limits (sum, product, quotient rules), and the chapter closes by computing, from first principles and then by rule, the derivatives of xnx^n, general polynomials, and sin⁡x\sin x, cos⁡x\cos x, tan⁡x\tan x.

The core ideas

From average velocity to instantaneous velocity — the intuitive idea

A body dropped from a cliff covers a distance s=4.9t2s = 4.9t^2 metres in tt seconds. The average velocity between two instants t1t_1 and t2t_2 is simply distance travelled divided by time elapsed, a quantity you have computed since middle school.

vˉ=s(t2)−s(t1)t2−t1.(1)\bar v = \frac{s(t_2)-s(t_1)}{t_2-t_1}. \qquad (1)

where: vˉ\bar v is the average velocity over the interval, and s(t)s(t) is the distance function. Computing vˉ\bar v for the interval t1=1.99t_1=1.99 to t2=2t_2=2 gives 19.551 m/s19.551\ \text{m/s}; for t1=1.999t_1=1.999 to t2=2t_2=2 it gives a number even closer to a fixed value. NCERT's own tables (12.2 and 12.3) push the starting point closer to t=2t=2 from both sides — from below (ending at t=2t=2) and from above (starting at t=2t=2) — and both sequences of average velocities squeeze toward the same number, somewhere between 19.55119.551 and 19.649 m/s19.649\ \text{m/s}. That common value, obtained by letting the time interval shrink to zero, is called the instantaneous velocity at t=2t=2, and it is exactly what the chapter will soon name the derivative of ss at t=2t=2. The geometric picture behind this arithmetic is the one that matters most for everything that follows. Plot ss against tt. The average velocity between t=2t=2 and a nearby instant t=2+ht=2+h is precisely the slope of the secant line joining the two points (2,s(2))(2, s(2)) and (2+h,s(2+h))(2+h, s(2+h)) on the graph. As hh shrinks toward 00, the second point slides along the curve toward the first, the secant line rotates, and in the limit it becomes the tangent line to the curve at t=2t=2. The instantaneous velocity is the slope of that tangent — a geometric fact that will reappear, unchanged, as the definition of the derivative in general.

Figure
A distance versus time graph for a falling body showing the secant line through two points on the curve rotating to become the tangent line as the second point slides toward the first, illustrating how average velocity becomes instantaneous velocity
Average velocity becomes instantaneous velocity as the secant becomes the tangent time t (s) distance s (m) s = 4.9 t squared A (t = 2, s = 19.6) B (t = 3, s = 44.1) secant AB — average velocity tangent at A — instantaneous velocity As the second point slides from B toward A, the secant rotates onto the tangent — the limiting slope is the derivative

Limits — left hand, right hand, and when they agree

The number a function is expected to take at x=ax=a, based on values of xx arbitrarily close to (but not equal to) aa, is called the limit of the function at aa. Because xx can approach aa from below or from above, two one-sided notions are needed first.

lim⁡x→a−f(x)andlim⁡x→a+f(x)(2)\lim_{x\to a^-} f(x) \quad \text{and} \quad \lim_{x\to a^+} f(x) \qquad (2)

where: the left hand limit lim⁡x→a−f(x)\lim_{x\to a^-} f(x) is the value dictated by points xx just less than aa, and the right hand limit lim⁡x→a+f(x)\lim_{x\to a^+} f(x) is the value dictated by points xx just greater than aa. The two-sided limit lim⁡x→af(x)\lim_{x\to a} f(x) exists, and equals that common value, exactly when the left and right hand limits coincide. Consider f(x)=1f(x) = 1 for x≤0x \le 0 and f(x)=2f(x)=2 for x>0x>0: the left hand limit at 00 is 11, the right hand limit is 22, they disagree, and so lim⁡x→0f(x)\lim_{x\to 0} f(x) simply does not exist — even though f(0)=1f(0)=1 is perfectly well defined. This example is the single cleanest illustration in the whole chapter that a function's value at a point and its limit at that point are two entirely different questions.

Figure
A step graph of a function equal to 1 for x less than or equal to zero and equal to 2 for x greater than zero, showing that the left hand limit and right hand limit at x equals zero are different so the two sided limit does not exist
Left and right hand limits disagree — the two sided limit does not exist x f(x) 0 f(x) = 1 for x ≤ 0 f(x) = 2 for x greater than 0 left hand limit = 1 right hand limit = 2 Since 1 is not equal to 2, the limit of f at x = 0 does not exist, although f(0) = 1 is defined.

The algebra of limits

Once two limits are known to exist, combinations of the two functions can be handled without recomputing anything from the definition. This is stated (without proof, as NCERT itself does) as a theorem.

lim⁡x→a[f(x)±g(x)]=lim⁡x→af(x)±lim⁡x→ag(x),lim⁡x→a[f(x) g(x)]=lim⁡x→af(x)⋅lim⁡x→ag(x),lim⁡x→af(x)g(x)=lim⁡x→af(x)lim⁡x→ag(x).(3)\lim_{x\to a}[f(x)\pm g(x)] = \lim_{x\to a} f(x) \pm \lim_{x\to a} g(x), \qquad \lim_{x\to a}[f(x)\,g(x)] = \lim_{x\to a} f(x)\cdot \lim_{x\to a} g(x), \qquad \lim_{x\to a}\frac{f(x)}{g(x)} = \frac{\lim_{x\to a} f(x)}{\lim_{x\to a} g(x)}. \qquad (3)

where: all three identities require lim⁡x→af(x)\lim_{x\to a} f(x) and lim⁡x→ag(x)\lim_{x\to a} g(x) to individually exist, and the quotient identity additionally needs lim⁡x→ag(x)≠0\lim_{x\to a} g(x) \ne 0. A useful special case: if gg is the constant function λ\lambda, then lim⁡x→a[λf(x)]=λlim⁡x→af(x)\lim_{x\to a}[\lambda f(x)] = \lambda \lim_{x\to a} f(x) — constants pull straight out of a limit. This theorem is the reason a limit of a complicated expression can be evaluated piece by piece rather than wrestled with as a whole.

Limits of polynomial and rational functions

Since lim⁡x→ax=a\lim_{x\to a} x = a trivially (the function f(x)=xf(x)=x approaches aa as xx approaches aa), repeated use of the product rule in (3)(3) gives lim⁡x→axn=an\lim_{x\to a} x^n = a^n for every positive integer nn, and then term-by-term use of the sum rule gives the limit of any polynomial.

f(x)=a0+a1x+a2x2+⋯+anxn   ⟹   lim⁡x→af(x)=a0+a1a+a2a2+⋯+anan=f(a).(4)f(x) = a_0 + a_1x + a_2x^2 + \cdots + a_nx^n \ \implies\ \lim_{x\to a} f(x) = a_0 + a_1a + a_2a^2 + \cdots + a_na^n = f(a). \qquad (4)

where: the striking conclusion is that for a polynomial, the limit at aa is simply the value of the polynomial at aa — direct substitution always works. For a rational function f(x)=g(x)h(x)f(x) = \frac{g(x)}{h(x)} with g,hg,h polynomials and h(a)≠0h(a)\ne 0, the quotient rule in (3)(3) gives lim⁡x→af(x)=g(a)h(a)\lim_{x\to a} f(x) = \frac{g(a)}{h(a)} just as directly. The interesting case, and the one that dominates exam questions, is h(a)=0h(a)=0. If also g(a)≠0g(a)\ne 0, the limit does not exist (the function blows up near aa). If both g(a)=0g(a)=0 and h(a)=0h(a)=0 — the 00\tfrac{0}{0} indeterminate form — then (x−a)(x-a) is a common factor of both gg and hh; write g(x)=(x−a)kg1(x)g(x)=(x-a)^k g_1(x) and h(x)=(x−a)ℓh1(x)h(x)=(x-a)^\ell h_1(x) with g1(a),h1(a)≠0g_1(a), h_1(a) \ne 0, cancel the common power of (x−a)(x-a) (legitimate since x≠ax\ne a throughout the limiting process), and evaluate what remains. If k>ℓk>\ell the limit is 00; if k=ℓk=\ell the limit is the finite ratio g1(a)/h1(a)g_1(a)/h_1(a); if k<ℓk<\ell the limit does not exist.

Limits of trigonometric functions — the sandwich theorem

Some limits cannot be settled by direct substitution or simple factoring; they need a squeeze. If a function g(x)g(x) is trapped between two other functions f(x)≤g(x)≤h(x)f(x)\le g(x)\le h(x) near aa, and ff and hh both approach the same limit at aa, then gg is forced to approach that same limit too — this is the sandwich theorem (Theorem 4).

f(x)≤g(x)≤h(x)  near a,lim⁡x→af(x)=l=lim⁡x→ah(x)   ⟹   lim⁡x→ag(x)=l.(5)f(x) \le g(x) \le h(x) \ \text{ near } a, \quad \lim_{x\to a} f(x) = l = \lim_{x\to a} h(x) \ \implies\ \lim_{x\to a} g(x) = l. \qquad (5)

where: ff, gg, hh share a common domain around aa, and ll is the common squeezed value. The chapter applies this once a geometric inequality is proved (in the first derivation below): cos⁡x<sin⁡xx<1\cos x < \frac{\sin x}{x} < 1 for 0<x<π20 < x < \frac{\pi}{2}. Since lim⁡x→0cos⁡x=1\lim_{x\to 0}\cos x = 1 and the constant function 11 trivially has limit 11, the sandwich theorem immediately forces lim⁡x→0sin⁡xx=1\lim_{x\to 0}\frac{\sin x}{x}=1. A companion identity, 1−cos⁡x=2sin⁡2 ⁣(x2)1-\cos x = 2\sin^2\!\left(\tfrac{x}{2}\right), converts this into the second standard trigonometric limit, proved in full in the second derivation below.

The derivative — definition and geometric meaning

Generalising the falling-stone calculation to any function ff and any point aa in its domain gives the formal definition of the derivative.

f′(a)=lim⁡h→0f(a+h)−f(a)h,provided the limit exists.(6)f'(a) = \lim_{h\to 0} \frac{f(a+h)-f(a)}{h}, \qquad \text{provided the limit exists.} \qquad (6)

where: f′(a)f'(a) is called the derivative of ff at aa, and this definition — a limit of a difference quotient — is called differentiation from first principles. The numerator f(a+h)−f(a)f(a+h)-f(a) is the change in the function's value, and hh is the change in xx; the ratio is an average rate of change over the interval from aa to a+ha+h, exactly as in (1)(1), and letting h→0h\to 0 converts that average rate into the instantaneous rate at aa. Geometrically, if P=(a,f(a))P=(a, f(a)) and Q=(a+h,f(a+h))Q=(a+h, f(a+h)) are two points on the graph of y=f(x)y=f(x), the difference quotient f(a+h)−f(a)h\frac{f(a+h)-f(a)}{h} is exactly the slope of the chord (secant) PQPQ. As h→0h\to 0, QQ slides along the curve toward PP and the secant PQPQ rotates into the tangent line at PP; hence f′(a)f'(a) equals the slope of the tangent to y=f(x)y=f(x) at the point (a,f(a))(a,f(a)) — the geometric fact previewed in the falling-stone picture above, now stated for any curve. The same rotating-secant picture drawn earlier for the falling stone applies unchanged to any curve y=f(x)y=f(x): replace the distance-time graph by the graph of ff, replace AA by P=(a,f(a))P=(a,f(a)), and replace the moving point by Q=(a+h,f(a+h))Q=(a+h, f(a+h)), and the secant-to-tangent limit is precisely f′(a)f'(a). Letting aa vary produces the derivative function f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x) = \lim_{h\to 0}\frac{f(x+h)-f(x)}{h}, defined wherever this limit exists (Definition 2). Common notations for the same object are ddxf(x)\frac{d}{dx}f(x), dydx\frac{dy}{dx} (when y=f(x)y=f(x)), Df(x)Df(x), and, for the value at a specific point, dfdx∣x=a\left.\frac{df}{dx}\right|_{x=a} or dfdx∣a\frac{df}{dx}\bigg|_a.

The algebra of derivatives

Because the derivative is itself defined through a limit, every algebra-of-limits rule in (3)(3) transfers directly to an algebra of derivatives (Theorem 5), stated here using u=f(x)u=f(x), v=g(x)v=g(x) for brevity.

(u±v)′=u′±v′,(uv)′=u′v+uv′,(uv)′=u′v−uv′v2  (v≠0).(7)(u\pm v)' = u'\pm v', \qquad (uv)' = u'v + uv', \qquad \left(\frac{u}{v}\right)' = \frac{u'v - uv'}{v^2}\ \ (v\ne 0). \qquad (7)

where: the middle identity is the Leibniz product rule: the derivative of a product is not the product of the derivatives, but the first function's derivative times the second, plus the first times the second's derivative. The last identity is the quotient rule: numerator's derivative times denominator, minus numerator times denominator's derivative, all divided by the denominator squared — the order in the numerator matters, since swapping it flips the sign. Both rules let a derivative be computed by combining known building-block derivatives instead of returning to the first-principles limit every time.

Standard derivatives

The single most useful building block is the derivative of xnx^n, proved in full in the third derivation below.

ddx(xn)=nxn−1 for any positive integer n;ddx(anxn+⋯+a1x+a0)=nanxn−1+⋯+2a2x+a1.(8)\frac{d}{dx}(x^n) = nx^{n-1} \ \text{for any positive integer } n; \qquad \frac{d}{dx}(a_nx^n+\cdots+a_1x+a_0) = na_nx^{n-1}+\cdots+2a_2x+a_1. \qquad (8)

where: the second identity (Theorem 7) follows from the first by the sum rule in (7)(7) applied term by term, and it is stated here for a general polynomial of degree nn with real coefficients a0,…,ana_0,\ldots,a_n. The result for xnx^n is stated for any real power in the chapter's remark, though only positive integer nn is proved. Alongside this, the fourth derivation below establishes the trigonometric derivatives.

ddx(sin⁡x)=cos⁡x,ddx(cos⁡x)=−sin⁡x,ddx(tan⁡x)=sec⁡2x.(9)\frac{d}{dx}(\sin x) = \cos x, \qquad \frac{d}{dx}(\cos x) = -\sin x, \qquad \frac{d}{dx}(\tan x) = \sec^2 x. \qquad (9)

where: these three, combined with the algebra of derivatives in (7)(7), generate the derivative of any combination of trigonometric functions — for instance cot⁡x=cos⁡xsin⁡x\cot x = \frac{\cos x}{\sin x} differentiates by the quotient rule to −csc⁡2x-\csc^2 x, and sin⁡2x=sin⁡xsin⁡x\sin^2 x = \sin x\sin x differentiates by the product rule to 2sin⁡xcos⁡x=sin⁡2x2\sin x\cos x = \sin 2x. The minus sign in ddx(cos⁡x)=−sin⁡x\frac{d}{dx}(\cos x) = -\sin x is the single most commonly dropped sign in this entire chapter.

Derivation AThe standard limit for powers of x

The goal of this derivation is to prove Theorem 2 of the chapter, the algebraic result lim⁡x→axn−anx−a=nan−1\lim_{x\to a}\dfrac{x^n-a^n}{x-a} = na^{n-1} for any positive integer nn, using nothing beyond ordinary polynomial division and the algebra of limits already established. This single result is what makes every polynomial and rational limit involving powers of xx tractable without ad-hoc factoring tricks, and it reappears immediately afterward as the engine of the derivative of xnx^n.

Step 1. Divide the polynomial xn−anx^n - a^n by x−ax - a. Polynomial long division confirms the standard factorisation xn−an=(x−a)(xn−1+xn−2a+xn−3a2+⋯+xan−2+an−1)x^n - a^n = (x-a)\left(x^{n-1} + x^{n-2}a + x^{n-3}a^2 + \cdots + xa^{n-2} + a^{n-1}\right), a sum of exactly nn terms, each of total degree n−1n-1 in xx and aa together.

Step 2. Divide both sides by (x−a)(x-a), valid since the limiting process only considers xx near aa but never equal to aa. This gives xn−anx−a=xn−1+xn−2a+xn−3a2+⋯+xan−2+an−1\dfrac{x^n-a^n}{x-a} = x^{n-1} + x^{n-2}a + x^{n-3}a^2 + \cdots + xa^{n-2} + a^{n-1} identically for all x≠ax\ne a — an exact algebraic identity, not yet a limit statement.

Step 3. Take the limit of both sides as x→ax\to a. The right side is a polynomial in xx (for fixed aa), so by the polynomial-limit result in (4)(4) its limit is obtained by direct substitution of x=ax=a: lim⁡x→a(xn−1+xn−2a+⋯+xan−2+an−1)=an−1+an−2⋅a+⋯+a⋅an−2+an−1\lim_{x\to a}\left(x^{n-1}+x^{n-2}a+\cdots+xa^{n-2}+a^{n-1}\right) = a^{n-1}+a^{n-2}\cdot a+\cdots+a\cdot a^{n-2}+a^{n-1}.

Step 4. Simplify. Every one of the nn terms from Step 3 equals an−1a^{n-1}, since an−1−k⋅ak=an−1a^{n-1-k}\cdot a^k = a^{n-1} for each k=0,1,…,n−1k=0,1,\ldots,n-1. Adding nn copies of an−1a^{n-1} gives nan−1na^{n-1}, so lim⁡x→axn−anx−a=nan−1\lim_{x\to a}\dfrac{x^n-a^n}{x-a} = na^{n-1}. NCERT remarks that the same formula holds when nn is any rational number and a>0a>0, a fact used freely later without re-proof. Verified: for n=15n=15, a=1a=1, all 1515 terms of Step 2 equal 114=11^{14}=1, summing to 1515, matching lim⁡x→1x15−1x−1=15\lim_{x\to1}\frac{x^{15}-1}{x-1}=15, used directly in the competitive worked example below.

Go deeper · Derivation B · 1 minThe sandwich theorem proof that sin x over x approaches 1
Derivation BThe sandwich theorem proof that sin x over x approaches 1

The goal here is to prove the two trigonometric limits in (9)(9)'s companion result, lim⁡x→0sin⁡xx=1\lim_{x\to 0}\frac{\sin x}{x}=1 and lim⁡x→01−cos⁡xx=0\lim_{x\to 0}\frac{1-\cos x}{x}=0, starting from a purely geometric comparison of areas in a unit circle and finishing with the sandwich theorem stated in (5)(5). No series expansion or calculus circularity is used — only elementary geometry of a circular sector and two triangles, exactly as NCERT presents it.

Step 1. Set up the geometric comparison. Let OO be the centre of a unit circle (OA=1OA=1), let AA and CC be points on the circle with angle AOC=xAOC=x radians, 0<x<π20<x<\frac{\pi}{2}, and drop perpendiculars: BABA perpendicular to OAOA at AA meeting line OCOC extended at BB, and CDCD perpendicular to OAOA at DD. Triangle OACOAC sits inside sector OACOAC, which sits inside triangle OABOAB, so Area(△OAC\triangle OAC) << Area(sector OACOAC) << Area(△OAB\triangle OAB).

Step 2. Compute each area. Triangle OACOAC has area 12(1)sin⁡x\frac12(1)\sin x, since CD=OCsin⁡x=sin⁡xCD=OC\sin x=\sin x. The sector has area x2π⋅π(OA)2=x2\frac{x}{2\pi}\cdot\pi(OA)^2=\frac{x}{2}. Triangle OABOAB has area 12tan⁡x\frac12\tan x, since AB=OAtan⁡x=tan⁡xAB=OA\tan x=\tan x. Substituting and cancelling 12\frac12: sin⁡x<x<tan⁡x\sin x < x < \tan x.

Step 3. Convert to the target form. Since sin⁡x>0\sin x>0 on 0<x<π20<x<\frac{\pi}{2}, dividing throughout by sin⁡x\sin x gives 1<xsin⁡x<1cos⁡x1<\dfrac{x}{\sin x}<\dfrac{1}{\cos x}; taking reciprocals reverses both inequalities to cos⁡x<sin⁡xx<1\cos x < \dfrac{\sin x}{x} < 1 — inequality (∗)(*) used earlier. Since sin⁡(−x)=−sin⁡x\sin(-x)=-\sin x and cos⁡(−x)=cos⁡x\cos(-x)=\cos x, the same inequality holds for −π2<x<0-\frac{\pi}{2}<x<0, so it holds on a full punctured neighbourhood of 00.

Step 4. Apply the sandwich theorem from (5)(5): since lim⁡x→0cos⁡x=1\lim_{x\to0}\cos x=1 and the constant 11 also has limit 11, lim⁡x→0sin⁡xx=1\lim_{x\to0}\dfrac{\sin x}{x}=1. For the second limit, use 1−cos⁡x=2sin⁡2 ⁣(x2)1-\cos x=2\sin^2\!\left(\frac{x}{2}\right): 1−cos⁡xx=sin⁡ ⁣(x2)⋅sin⁡(x/2)x/2\dfrac{1-\cos x}{x}=\sin\!\left(\frac{x}{2}\right)\cdot\dfrac{\sin(x/2)}{x/2}. As x→0x\to0, x2→0\frac{x}{2}\to0, so sin⁡(x/2)x/2→1\dfrac{\sin(x/2)}{x/2}\to1 by Step 4's first result, while sin⁡(x/2)→0\sin(x/2)\to0; by the product rule for limits, lim⁡x→01−cos⁡xx=0×1=0\lim_{x\to0}\dfrac{1-\cos x}{x}=0\times1=0. Verified numerically: at x=0.01x=0.01 radians, sin⁡x/x=0.999983…≈1\sin x/x = 0.999983\ldots \approx 1 and (1−cos⁡x)/x=0.005≈0(1-\cos x)/x = 0.005 \approx 0, both consistent with the proved limits.

Go deeper · Derivation C · 1 minThe derivative of x to the power n from first principles
Derivation CThe derivative of x to the power n from first principles

The goal of this derivation is to prove Theorem 6, ddx(xn)=nxn−1\dfrac{d}{dx}(x^n)=nx^{n-1} for any positive integer nn, starting from the first-principles definition (6)(6) and the binomial theorem — the single most-used differentiation formula in the entire syllabus, and the one every polynomial derivative in (8)(8) ultimately rests on. A second, independent proof by induction and the product rule is given at the end, since NCERT presents both and the two illuminate different aspects of the result.

Step 1. Write the first-principles definition for f(x)=xnf(x)=x^n: f′(x)=lim⁡h→0(x+h)n−xnhf'(x) = \lim_{h\to 0}\dfrac{(x+h)^n - x^n}{h}.

Step 2. Expand (x+h)n(x+h)^n using the binomial theorem: (x+h)n=nC0 xn+nC1 xn−1h+nC2 xn−2h2+⋯+nCn hn(x+h)^n = {}^{n}C_0\,x^n + {}^{n}C_1\,x^{n-1}h + {}^{n}C_2\,x^{n-2}h^2 + \cdots + {}^{n}C_n\,h^n. Since nC0=1^{n}C_0=1, subtracting xnx^n gives (x+h)n−xn=nC1 xn−1h+nC2 xn−2h2+⋯+hn(x+h)^n - x^n = {}^{n}C_1\,x^{n-1}h + {}^{n}C_2\,x^{n-2}h^2 + \cdots + h^n, factored as h(nxn−1+nC2 xn−2h+⋯+hn−1)h\left(nx^{n-1} + {}^{n}C_2\,x^{n-2}h+\cdots + h^{n-1}\right), using nC1=n^{n}C_1=n.

Step 3. Substitute into the difference quotient and cancel the common factor of hh (valid since h≠0h\ne 0 throughout the limiting process): (x+h)n−xnh=nxn−1+nC2 xn−2h+⋯+hn−1\dfrac{(x+h)^n-x^n}{h} = nx^{n-1} + {}^{n}C_2\,x^{n-2}h + \cdots + h^{n-1}. Every term after the first carries at least one positive power of hh.

Step 4. Take the limit as h→0h\to 0; every term with a positive power of hh vanishes, leaving f′(x)=nxn−1f'(x)=nx^{n-1}. As an independent check, induction also works: the base case n=1n=1 gives ddx(x)=lim⁡h→0(x+h)−xh=1\frac{d}{dx}(x)=\lim_{h\to0}\frac{(x+h)-x}{h}=1; assuming ddx(xn−1)=(n−1)xn−2\frac{d}{dx}(x^{n-1})=(n-1)x^{n-2} and writing xn=x⋅xn−1x^n=x\cdot x^{n-1}, the product rule from (7)(7) gives ddx(xn)=1⋅xn−1+x⋅(n−1)xn−2=nxn−1\frac{d}{dx}(x^n) = 1\cdot x^{n-1}+x\cdot(n-1)x^{n-2} = nx^{n-1}, matching Step 4 and completing the induction. Verified: for n=2n=2, Step 2 to 4 gives (x+h)2−x2h=2xh+h2h=2x+h→2x\frac{(x+h)^2-x^2}{h} = \frac{2xh+h^2}{h} = 2x+h \to 2x as h→0h\to0, matching nxn−1=2x1nx^{n-1}=2x^1; direct product-rule computation of x⋅xx\cdot x also gives 1⋅x+x⋅1=2x1\cdot x + x\cdot 1 = 2x.

Go deeper · Derivation D · 1 minThe derivative of sin x from first principles
Derivation DThe derivative of sin x from first principles

The goal of this derivation is to compute ddx(sin⁡x)\dfrac{d}{dx}(\sin x) directly from the definition (6)(6), using a sum-to-product trigonometric identity and the two standard trigonometric limits proved above, and then to show that an identical method yields ddx(cos⁡x)=−sin⁡x\dfrac{d}{dx}(\cos x)=-\sin x — together these two results, combined with the quotient rule, immediately give ddx(tan⁡x)=sec⁡2x\dfrac{d}{dx}(\tan x)=\sec^2x as stated in (9)(9).

Step 1. Write the first-principles definition for f(x)=sin⁡xf(x)=\sin x: f′(x)=lim⁡h→0sin⁡(x+h)−sin⁡xhf'(x) = \lim_{h\to 0}\dfrac{\sin(x+h)-\sin x}{h}. Use the sum-to-product identity sin⁡A−sin⁡B=2cos⁡ ⁣(A+B2)sin⁡ ⁣(A−B2)\sin A - \sin B = 2\cos\!\left(\frac{A+B}{2}\right)\sin\!\left(\frac{A-B}{2}\right) with A=x+hA=x+h, B=xB=x: sin⁡(x+h)−sin⁡x=2cos⁡ ⁣(x+h2)sin⁡ ⁣(h2)\sin(x+h)-\sin x = 2\cos\!\left(x+\frac{h}{2}\right)\sin\!\left(\frac{h}{2}\right).

Step 2. Substitute into the difference quotient and regroup the 22 with the hh in the denominator: f′(x)=lim⁡h→0cos⁡ ⁣(x+h2)⋅sin⁡(h/2)h/2f'(x) = \lim_{h\to 0}\cos\!\left(x+\frac{h}{2}\right)\cdot \dfrac{\sin(h/2)}{h/2}.

Step 3. Take the limit of each factor separately using the product rule for limits in (3)(3). As h→0h\to 0, cos⁡ ⁣(x+h2)→cos⁡x\cos\!\left(x+\frac{h}{2}\right) \to \cos x by direct substitution, and h2→0\frac{h}{2}\to 0, so by the sandwich-theorem result proved above, sin⁡(h/2)h/2→1\dfrac{\sin(h/2)}{h/2} \to 1.

Step 4. Multiply the two limits: f′(x)=cos⁡x⋅1=cos⁡xf'(x) = \cos x \cdot 1 = \cos x, establishing ddx(sin⁡x)=cos⁡x\dfrac{d}{dx}(\sin x)=\cos x. The identical method, starting from cos⁡(x+h)−cos⁡x=−2sin⁡ ⁣(x+h2)sin⁡ ⁣(h2)\cos(x+h)-\cos x = -2\sin\!\left(x+\frac{h}{2}\right)\sin\!\left(\frac{h}{2}\right), gives ddx(cos⁡x)=−sin⁡x⋅1=−sin⁡x\dfrac{d}{dx}(\cos x) = -\sin x \cdot 1 = -\sin x. Finally, writing tan⁡x=sin⁡xcos⁡x\tan x = \dfrac{\sin x}{\cos x} and applying the quotient rule from (7)(7): ddx(tan⁡x)=cos⁡x⋅cos⁡x−sin⁡x⋅(−sin⁡x)cos⁡2x=cos⁡2x+sin⁡2xcos⁡2x=sec⁡2x\dfrac{d}{dx}(\tan x) = \dfrac{\cos x\cdot\cos x - \sin x\cdot(-\sin x)}{\cos^2 x} = \dfrac{\cos^2x+\sin^2x}{\cos^2x} = \sec^2 x, completing the trio in (9)(9). Verified: at x=0x=0, ddx(sin⁡x)∣x=0=cos⁡0=1\frac{d}{dx}(\sin x)|_{x=0}=\cos 0 = 1, matching NCERT's direct computation lim⁡h→0sin⁡hh=1\lim_{h\to0}\frac{\sin h}{h}=1; at x=0x=0, ddx(cos⁡x)∣x=0=−sin⁡0=0\frac{d}{dx}(\cos x)|_{x=0}=-\sin 0=0.

Worked examples

Board level - evaluating a limit that reduces to the 0/0 form (NCERT Example 2)

Evaluate lim⁡x→2x3−4x2+4xx2−4\displaystyle\lim_{x\to 2} \dfrac{x^3-4x^2+4x}{x^2-4}.

Step 1. Check direct substitution first: at x=2x=2, the numerator is 8−16+8=08-16+8=0 and the denominator is 4−4=04-4=0, a 00\tfrac{0}{0} indeterminate form, so direct substitution fails and factoring is needed.

Step 2. Factor both numerator and denominator to expose the common factor (x−2)(x-2). The numerator x3−4x2+4x=x(x2−4x+4)=x(x−2)2x^3-4x^2+4x = x(x^2-4x+4) = x(x-2)^2. The denominator x2−4=(x+2)(x−2)x^2-4 = (x+2)(x-2).

Step 3. Cancel the common factor (x−2)(x-2), valid because x≠2x\ne 2 throughout the limiting process: x(x−2)2(x+2)(x−2)=x(x−2)x+2\dfrac{x(x-2)^2}{(x+2)(x-2)} = \dfrac{x(x-2)}{x+2} for x≠2x\ne 2. This new expression has no remaining 00\tfrac{0}{0} obstruction at x=2x=2.

Step 4. Substitute x=2x=2 into the simplified expression: 2(2−2)2+2=2(0)4=0\dfrac{2(2-2)}{2+2} = \dfrac{2(0)}{4} = 0. Answer: lim⁡x→2x3−4x2+4xx2−4=0\displaystyle\lim_{x\to 2} \dfrac{x^3-4x^2+4x}{x^2-4} = 0.

Board level - finding a derivative from first principles (NCERT Example 6)

Find the derivative of f(x)=2x2+3x−5f(x) = 2x^2+3x-5 at x=−1x=-1, and verify that f′(0)+3f′(−1)=0f'(0)+3f'(-1)=0.

Step 1. Write the first-principles definition at x=−1x=-1: f′(−1)=lim⁡h→0f(−1+h)−f(−1)hf'(-1) = \lim_{h\to0}\dfrac{f(-1+h)-f(-1)}{h}. Compute f(−1+h)=2(−1+h)2+3(−1+h)−5=2(1−2h+h2)−3+3h−5=2−4h+2h2−3+3h−5=2h2−h−6f(-1+h) = 2(-1+h)^2+3(-1+h)-5 = 2(1-2h+h^2)-3+3h-5 = 2-4h+2h^2-3+3h-5 = 2h^2-h-6, and f(−1)=2(1)−3−5=−6f(-1) = 2(1)-3-5=-6.

Step 2. Subtract and divide: f′(−1)=lim⁡h→0(2h2−h−6)−(−6)h=lim⁡h→02h2−hh=lim⁡h→0(2h−1)=−1f'(-1) = \lim_{h\to0}\dfrac{(2h^2-h-6)-(-6)}{h} = \lim_{h\to0}\dfrac{2h^2-h}{h} = \lim_{h\to0}(2h-1) = -1, cancelling the common factor of hh before taking the limit.

Step 3. Repeat the process at x=0x=0: f(0+h)=f(h)=2h2+3h−5f(0+h)=f(h)=2h^2+3h-5 and f(0)=−5f(0)=-5, so f′(0)=lim⁡h→0(2h2+3h−5)−(−5)h=lim⁡h→02h2+3hh=lim⁡h→0(2h+3)=3f'(0) = \lim_{h\to0}\dfrac{(2h^2+3h-5)-(-5)}{h} = \lim_{h\to0}\dfrac{2h^2+3h}{h} = \lim_{h\to0}(2h+3) = 3.

Step 4. Verify the stated identity: f′(0)+3f′(−1)=3+3(−1)=3−3=0f'(0)+3f'(-1) = 3+3(-1) = 3-3=0, exactly as claimed. Answer: f′(−1)=−1f'(-1) = -1, f′(0)=3f'(0)=3, and f′(0)+3f′(−1)=0f'(0)+3f'(-1)=0.

Competitive level (JEE / NEET) - a standard-limit shortcut for a ratio of powers (NCERT Example 3(i))

Evaluate lim⁡x→1x15−1x10−1\displaystyle\lim_{x\to 1}\dfrac{x^{15}-1}{x^{10}-1}.

Step 1. Recognise the 00\tfrac{0}{0} form (both numerator and denominator vanish at x=1x=1) and rewrite the ratio to expose two instances of the standard limit lim⁡x→axn−anx−a=nan−1\lim_{x\to a}\frac{x^n-a^n}{x-a}=na^{n-1} from the first derivation, using a=1a=1: x15−1x10−1=x15−1x−1/x10−1x−1\dfrac{x^{15}-1}{x^{10}-1} = \dfrac{x^{15}-1}{x-1}\Big/\dfrac{x^{10}-1}{x-1}, dividing and multiplying by (x−1)(x-1).

Step 2. Split the limit of the quotient using the algebra of limits, since both individual limits exist: lim⁡x→1x15−1x10−1=lim⁡x→1x15−1x−1lim⁡x→1x10−1x−1\lim_{x\to1}\dfrac{x^{15}-1}{x^{10}-1} = \dfrac{\lim_{x\to1}\frac{x^{15}-1}{x-1}}{\lim_{x\to1}\frac{x^{10}-1}{x-1}}.

Step 3. Apply the standard limit to each piece with a=1a=1: lim⁡x→1x15−1x−1=15(1)14=15\lim_{x\to1}\dfrac{x^{15}-1}{x-1} = 15(1)^{14}=15 and lim⁡x→1x10−1x−1=10(1)9=10\lim_{x\to1}\dfrac{x^{10}-1}{x-1} = 10(1)^{9}=10.

Step 4. Divide the two results: 1510=32\dfrac{15}{10} = \dfrac{3}{2}. Answer: lim⁡x→1x15−1x10−1=32\displaystyle\lim_{x\to 1}\dfrac{x^{15}-1}{x^{10}-1} = \dfrac{3}{2}. Timing note: under a minute. The instant a limit of the form xm−1xn−1\frac{x^m-1}{x^n-1} (or more generally xm−amxn−an\frac{x^m-a^m}{x^n-a^n}) appears at x→ax\to a, skip factoring entirely and go straight to the ratio m am−1n an−1\frac{m\,a^{m-1}}{n\,a^{n-1}} — here 15(1)1410(1)9=1510=32\frac{15(1)^{14}}{10(1)^9}=\frac{15}{10}=\frac32 in one line. The only trap is applying the standard limit formula when the exponent is not a plain positive integer power of xx alone (for example if the base itself were x2x^2 rather than xx) — check the form matches xn−anx−a\frac{x^n-a^n}{x-a} exactly before shortcutting.

Competitive level (JEE / NEET) - trigonometric limits by algebraic manipulation (NCERT Example 4)

Evaluate (a) lim⁡x→0sin⁡4xsin⁡2x\displaystyle\lim_{x\to 0}\dfrac{\sin 4x}{\sin 2x} and (b) lim⁡x→0tan⁡xx\displaystyle\lim_{x\to 0}\dfrac{\tan x}{x}.

Step 1. For part (a), multiply and divide to create the standard form sin⁡θθ\frac{\sin\theta}{\theta} in both numerator and denominator: sin⁡4xsin⁡2x=sin⁡4x4x⋅2xsin⁡2x⋅4x2x=sin⁡4x4x/sin⁡2x2x⋅2\dfrac{\sin 4x}{\sin 2x} = \dfrac{\sin 4x}{4x}\cdot\dfrac{2x}{\sin 2x}\cdot\dfrac{4x}{2x} = \dfrac{\sin4x}{4x}\Big/\dfrac{\sin2x}{2x}\cdot 2, regrouping so that 4x→04x\to0 and 2x→02x\to0 exactly when x→0x\to0.

Step 2. Apply the algebra of limits and the standard result lim⁡θ→0sin⁡θθ=1\lim_{\theta\to0}\frac{\sin\theta}{\theta}=1 from the second derivation, to each factor separately: lim⁡x→0sin⁡4x4x=1\lim_{x\to0}\dfrac{\sin4x}{4x}=1 and lim⁡x→0sin⁡2x2x=1\lim_{x\to0}\dfrac{\sin2x}{2x}=1, since as x→0x\to0 both 4x→04x\to0 and 2x→02x\to0.

Step 3. Combine: lim⁡x→0sin⁡4xsin⁡2x=2⋅lim⁡x→0sin⁡4x4xlim⁡x→0sin⁡2x2x=2⋅11=2\displaystyle\lim_{x\to0}\dfrac{\sin4x}{\sin2x} = 2\cdot\dfrac{\lim_{x\to0}\frac{\sin4x}{4x}}{\lim_{x\to0}\frac{\sin2x}{2x}} = 2\cdot\dfrac{1}{1} = 2. For part (b), write tan⁡x=sin⁡xcos⁡x\tan x = \dfrac{\sin x}{\cos x}, so tan⁡xx=sin⁡xx⋅1cos⁡x\dfrac{\tan x}{x} = \dfrac{\sin x}{x}\cdot\dfrac{1}{\cos x}.

Step 4. Take the limit of the product using (3)(3): lim⁡x→0sin⁡xx=1\lim_{x\to0}\dfrac{\sin x}{x}=1 and lim⁡x→01cos⁡x=1cos⁡0=11=1\lim_{x\to0}\dfrac{1}{\cos x} = \dfrac{1}{\cos 0}=\dfrac{1}{1}=1, so lim⁡x→0tan⁡xx=1×1=1\lim_{x\to0}\dfrac{\tan x}{x} = 1\times1=1. Answer: (a) lim⁡x→0sin⁡4xsin⁡2x=2\displaystyle\lim_{x\to 0}\dfrac{\sin 4x}{\sin 2x}=2 and (b) lim⁡x→0tan⁡xx=1\displaystyle\lim_{x\to 0}\dfrac{\tan x}{x}=1. Timing note: about ninety seconds for both parts together. The reflex to build is: whenever you see sin⁡(kx)\sin(kx) or tan⁡(kx)\tan(kx) over xx (or over another sin⁡\sin or tan⁡\tan expression), multiply and divide by the coefficient kk inside the argument to force the exact pattern sin⁡(kx)kx→1\frac{\sin(kx)}{kx}\to1; never apply lim⁡sin⁡xx=1\lim\frac{\sin x}{x}=1 to sin⁡4xx\frac{\sin 4x}{x} directly without first inserting the missing factor of 44. A frequent slip under time pressure is forgetting the leftover multiplicative constant (the 22 in part (a)) after the two standard-limit factors have been extracted.

Common traps

Stopping at 00\tfrac00. A 00\tfrac00 result is not the answer — it signals a common factor (x−a)(x-a) that must be found and cancelled before substituting again. Never report "00\frac00" or "undefined" without first attempting to factor.

Treating f(a)f(a) and lim⁡x→af(x)\lim_{x\to a} f(x) as automatically equal. They coincide for "nice" functions like polynomials, but the piecewise example above shows a function whose value is defined while its limit is not, and vice versa. Always answer the exact question asked.

Ignoring left and right hand limits for piecewise functions. Whenever ff changes formula at x=ax=a, compute lim⁡x→a−f(x)\lim_{x\to a^-} f(x) and lim⁡x→a+f(x)\lim_{x\to a^+} f(x) separately, and only claim the two-sided limit exists if they match exactly.

Forgetting the quotient rule's minus sign and squared denominator. (uv)′=u′v−uv′v2\left(\frac{u}{v}\right)' = \frac{u'v-uv'}{v^2}, not u′v+uv′v2\frac{u'v+uv'}{v^2} and not over plain vv — both slips are common under exam pressure.

Misremembering the sign of ddx(cos⁡x)\frac{d}{dx}(\cos x). It is −sin⁡x-\sin x, not +sin⁡x+\sin x; the derivation above shows the minus sign comes from the identity cos⁡A−cos⁡B=−2sin⁡(⋯ )sin⁡(⋯ )\cos A-\cos B=-2\sin(\cdots)\sin(\cdots).

Applying lim⁡xn−anx−a=nan−1\lim\frac{x^n-a^n}{x-a}=na^{n-1} to a pattern that does not actually match, such as xn−amx−a\frac{x^n-a^m}{x-a} with n≠mn\ne m, or a base other than plain xx. Check exponents and base before shortcutting; when in doubt, factor directly as in the first worked example.

You should be able to…

  • Evaluate lim⁡x→af(x)\lim_{x\to a} f(x) for polynomial functions by direct substitution, using the result that a polynomial's limit equals its value at aa.
  • Recognise a 00\tfrac{0}{0} indeterminate form in a rational function's limit, factor out the common (x−a)(x-a), and evaluate the simplified expression.
  • State the left hand limit and right hand limit of a piecewise function, and correctly decide whether the two-sided limit exists.
  • Apply the algebra of limits (sum, difference, product, quotient) to break a compound limit into simpler pieces that can be evaluated separately.
  • Use the standard result lim⁡x→axn−anx−a=nan−1\lim_{x\to a}\frac{x^n-a^n}{x-a}=na^{n-1} to shortcut limits built from powers, including ratios like xm−1xn−1\frac{x^m-1}{x^n-1}.
  • Evaluate trigonometric limits at 00 using lim⁡x→0sin⁡xx=1\lim_{x\to0}\frac{\sin x}{x}=1 and lim⁡x→01−cos⁡xx=0\lim_{x\to0}\frac{1-\cos x}{x}=0, inserting missing multiplicative constants where needed.
  • Compute a derivative from first principles, f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x)=\lim_{h\to0}\frac{f(x+h)-f(x)}{h}, for polynomial and simple trigonometric functions.
  • Interpret f′(a)f'(a) geometrically as the slope of the tangent line to y=f(x)y=f(x) at x=ax=a, and connect it to the idea of instantaneous rate of change.
  • Apply the sum, Leibniz product, and quotient rules to differentiate combinations of functions without returning to first principles every time.
  • Differentiate xnx^n, general polynomials, sin⁡x\sin x, cos⁡x\cos x and tan⁡x\tan x fluently, both from the standard formulas and, when asked, from first principles.

Ask the tutor: Want to work through a first-principles derivative or a tricky 0/0 limit together, step by step?

Why does the limit at x equals a not care what happens exactly at x equals a?

Because a limit describes a trend in the values of f(x) for x close to a but never equal to a, not a single evaluation at a. The formal left and right hand limits are both built entirely from points near a, deliberately excluding a itself. This is exactly why a function can have a limit at a point where it is not even defined, such as x2−4x−2\frac{x^2-4}{x-2} at x=2x=2, and why a function can be defined at a point while its limit there fails to exist, as in the step-function example in the core ideas above. The value f(a), if it exists, is a separate fact that the limit simply does not consult.

Why can we cancel the factor x minus a from the numerator and denominator when a limit gives 0 over 0?

Because throughout the entire limiting process x is only ever taken near a, never equal to a, so x−ax-a is never actually zero and dividing by it is always legitimate. Once you write g(x)=(x−a)g1(x)g(x)=(x-a)g_1(x) and h(x)=(x−a)h1(x)h(x)=(x-a)h_1(x), the identity g(x)h(x)=g1(x)h1(x)\frac{g(x)}{h(x)}=\frac{g_1(x)}{h_1(x)} holds for every x≠ax\ne a, which is exactly the set of points a limit examines. After cancelling, you evaluate the simplified expression at x=ax=a using ordinary substitution, since g1g_1 and h1h_1 are typically well behaved there even though the original ratio was not.

Is dy by dx a fraction, and can I split it into dy and dx separately?

Not at this stage. dydx\frac{dy}{dx} is a single symbol denoting the derivative, defined as the limit lim⁡h→0f(x+h)−f(x)h\lim_{h\to0}\frac{f(x+h)-f(x)}{h}, and it should be treated as one indivisible object here, not as an actual fraction with a numerator dy and a denominator dx that can be manipulated separately. It behaves suggestively like a fraction (the quotient and product rules even look like fraction algebra), which is a useful mnemonic, but formally justifying dy and dx as separate quantities that can be split apart belongs to later, more careful treatments of calculus, not to this first-principles chapter.

Why is the limit of sin x over x equal to 1 only when x is measured in radians?

The geometric proof above rests on the inequality sin⁡x<x<tan⁡x\sin x < x < \tan x, which compares an actual arc length (the radian measure xx) against straight-line lengths sin⁡x\sin x and tan⁡x\tan x on a unit circle — the comparison is only valid because radian measure is itself defined as arc length divided by radius. If xx were measured in degrees, the same geometric picture would introduce an extra constant factor of π180\frac{\pi}{180}, so the limit would instead approach π180\frac{\pi}{180}, not 11. Every trigonometric limit and derivative in this chapter silently assumes radian measure for exactly this reason.

What is the actual difference between average velocity and instantaneous velocity, and how does the derivative connect them?

Average velocity is distance travelled divided by time elapsed over some finite interval, such as from t=1.99t=1.99 to t=2t=2 seconds — it is a single number attached to an interval, not to an instant. Instantaneous velocity is what that average velocity settles down to as the interval is shrunk toward a single instant, and the derivative s′(t)=lim⁡h→0s(t+h)−s(t)hs'(t)=\lim_{h\to0}\frac{s(t+h)-s(t)}{h} is the formal name for exactly this limiting process. In other words, instantaneous velocity is not a different kind of quantity from average velocity; it is the limit of average velocities taken over intervals that shrink to zero length, which is precisely why the chapter introduces limits before it ever defines the derivative.

Before this

Where this leads