Calculus · ClipSAT

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Calculus

Level · High school → introductory college · Calc I–III Chapters · 16 Explorers · 15 interactive Prerequisite · Algebra & functions
0

Foundations & Precalculus Review

Calculus is the study of how functions change and accumulate, so every later idea leans on fluency with functions themselves. This chapter gathers the algebra, function families, and notation the rest of the course quietly assumes.

● Definition 0.1 — Function, domain, range

A function f f assigns to each input x x in its domain exactly one output f(x) f(x) . The set of resulting outputs is the range. We write f:R→R f:\mathbb{R}\to\mathbb{R} for a real-valued function of a real variable.

The function toolkit

A handful of parent functions, combined and transformed, generate almost everything in single-variable calculus.

Power
xn x^{n}
Exponential
ax, ex a^{x},\ e^{x}
Logarithm
log⁡ax, ln⁡x \log_a x,\ \ln x
Trigonometric
sin⁡x, cos⁡x, tan⁡x \sin x,\ \cos x,\ \tan x
● Definition 0.2 — Transformations

From a parent f f , the graph of y=a f(x−h)+k y=a\,f(x-h)+k is shifted right by h h , up by k k , and scaled vertically by a a (reflected across the x x -axis when a<0 a\lt 0 ).

⊙ Explorer · Transform a parent functioninteractive
vertex (h, 0)(0.0, 0)
directionopens up

The faint grey curve is the parent y=x2y=x^2; the bold curve is y=a(x−h)2y=a(x-h)^2. Watch the vertex slide and flip.

Exponentials and logarithms

These are inverse operations, and their algebra appears constantly in growth models and integration. The key laws:

log⁡a(xy)=log⁡ax+log⁡ay,log⁡a ⁣(xy)=log⁡ax−log⁡ay,log⁡a(xr)=rlog⁡ax. \log_a(xy)=\log_a x+\log_a y, \qquad \log_a\!\Big(\tfrac{x}{y}\Big)=\log_a x-\log_a y, \qquad \log_a(x^{r})=r\log_a x.

The natural base e≈2.71828 e\approx 2.71828 makes ddxex=ex \dfrac{d}{dx}e^{x}=e^{x} , which is why it dominates calculus.

Worked example 0.A — Finding a domain

Find the domain of f(x)=x−2x−5 \displaystyle f(x)=\frac{\sqrt{x-2}}{x-5} .

The square root needs x−2≥0 x-2\ge 0 , so x≥2 x\ge 2 ; the denominator forbids x=5 x=5 . Combining,

domain=[2,5)∪(5,∞). \text{domain}=[2,5)\cup(5,\infty).

Worked example 0.B — Reading a transformation

Describe y=−2(x−3)2+1 y=-2(x-3)^{2}+1 relative to y=x2 y=x^{2} .

It is shifted right 3 3 and up 1 1 , stretched vertically by 2 2 , and reflected (since a=−2<0 a=-2\lt 0 ). The vertex is (3,1) (3,1) and the parabola opens downward.

Coordinate plane with graph of y = x^2, y = -(x - 2)^2 + 3; marked points (0, 0) (0, 0), Vertex (2, 3) (2, 3)-2-11234-224xyy = x²y = -(x − 2)² + 3(0, 0)Vertex (2, 3)
Parent parabola y=x2y = x^2 alongside shifted and inverted parabola y=−(x−2)2+3y = -(x - 2)^2 + 3 with vertex at (2,3)(2, 3).
⚠ Common Traps & Exam Pitfalls
The 'Universal Distributive' Fallacy: Square roots, powers, and logs NEVER distribute across addition:
• a2+b2≠a+b\sqrt{a^2 + b^2} \ne a + b
• (a+b)2≠a2+b2(a + b)^2 \ne a^2 + b^2 (remember the middle term 2ab2ab!)
• 1a+b≠1a+1b\frac{1}{a + b} \ne \frac{1}{a} + \frac{1}{b}
• ln⁡(a+b)≠ln⁡a+ln⁡b\ln(a + b) \ne \ln a + \ln b.

Domain Restrictions: In calculus, domains govern continuity and differentiability. Always inspect: (1) Even roots: radicand must be ≥0\ge 0; (2) Denominators: must be ≠0\ne 0; (3) Logarithms: argument must be strictly >0> 0.
Find the domain of f(x)=ln⁡(x+3)4−x2f(x) = \dfrac{\ln(x + 3)}{\sqrt{4 - x^2}}.
For the numerator, the logarithm requires x+3>0  ⟹  x>−3x + 3 > 0 \implies x > -3. For the denominator, the square root in the denominator requires 4−x2>0  ⟹  x2<4  ⟹  −2<x<24 - x^2 > 0 \implies x^2 < 4 \implies -2 < x < 2. Taking the intersection of x>−3x > -3 and −2<x<2-2 < x < 2 gives the domain (−2,2)(-2, 2).
📝 Chapter Quiz
1

Limits & Continuity

Calculus rests on a single idea: what value does a function approach as its input creeps toward a target? It need not ever reach that value — what matters is the trend.

● Definition 1.1 — Limit (informal)

We write lim⁡x→cf(x)=L \displaystyle \lim_{x \to c} f(x) = L if the outputs f(x) f(x) can be made as close to L L as we like by taking x x sufficiently close to c c (but not equal to c c ).

The function may even be undefined exactly at c c . Consider f(x)=x2−1x−1 \displaystyle f(x)=\frac{x^2-1}{x-1} . At x=1 x=1 the formula gives 00 \tfrac{0}{0} , yet factoring reveals f(x)=x+1 f(x)=x+1 everywhere else, so the curve heads straight for 2 2 .

⊙ Explorer · Approaching a limitinteractive
input  x0.500
output  f(x)1.500
limit as x→12.000

Slide from either side: f(x)f(x) marches to 22, even though the point at x=1x=1 is a hole.

One-sided limits

Sometimes the approach differs by direction. The left-hand limit lim⁡x→c−f(x) \displaystyle \lim_{x\to c^-} f(x) and right-hand limit lim⁡x→c+f(x) \displaystyle \lim_{x\to c^+} f(x) must agree for the two-sided limit to exist:

lim⁡x→cf(x)=L⟺lim⁡x→c−f(x)=lim⁡x→c+f(x)=L. \lim_{x\to c} f(x)=L \quad\Longleftrightarrow\quad \lim_{x\to c^-}f(x)=\lim_{x\to c^+}f(x)=L.

● Definition 1.2 — Continuity

A function f f is continuous at c c when all three hold: (i) f(c) f(c) is defined, (ii) lim⁡x→cf(x) \displaystyle\lim_{x\to c} f(x) exists, and (iii) the two are equal, lim⁡x→cf(x)=f(c) \displaystyle\lim_{x\to c} f(x)=f(c) . Informally: you can draw it through c c without lifting the pen.

Two limits worth memorising

Trig squeeze
lim⁡x→0sin⁡xx=1 \displaystyle \lim_{x\to 0}\frac{\sin x}{x}=1
The number e
lim⁡x→∞ ⁣(1+1x)x=e \displaystyle \lim_{x\to\infty}\!\Big(1+\tfrac1x\Big)^{x}=e
Worked example 1.A

Evaluate lim⁡x→3x2−9x−3 \displaystyle \lim_{x\to 3}\frac{x^2-9}{x-3} .

Direct substitution gives 00 \tfrac00 , so factor the numerator: x2−9=(x−3)(x+3) x^2-9=(x-3)(x+3) . Cancel the common factor (valid since x≠3 x\neq 3 in the limit):

lim⁡x→3(x−3)(x+3)x−3=lim⁡x→3(x+3)=6. \lim_{x\to 3}\frac{(x-3)(x+3)}{x-3}=\lim_{x\to 3}(x+3)=6.

Coordinate plane with graph of f(x) = (x^2 - 9)/(x - 3); marked points Hole (3, 6) (3, 6)123452468xyf(x) = (x² − 9)/(x − 3)Hole (3, 6)
Plot of rational function f(x)=x2−9x−3f(x) = \frac{x^2 - 9}{x - 3} showing a removable discontinuity (hole) at (3,6)(3, 6).
⚠ Common Traps & Exam Pitfalls
Indeterminate Form 0/0: Obtaining 00\frac{0}{0} from direct substitution does NOT mean the limit is 0, 1, or does not exist. It is an indeterminate form signaling that an algebraic simplification (factoring, conjugate rationalization, trig identity, or L'Hôpital's Rule) must be performed.

Two-Sided Limit Existence: The overall limit lim⁡x→cf(x)=L\lim_{x\to c} f(x) = L exists IF AND ONLY IF both one-sided limits exist and agree: lim⁡x→c−f(x)=lim⁡x→c+f(x)=L\lim_{x\to c^-} f(x) = \lim_{x\to c^+} f(x) = L. For piece-wise and absolute value functions, always verify both directions separately.

Continuity Checklist: A function ff is continuous at x=cx = c only if all 3 conditions hold: (1) f(c)f(c) is defined; (2) lim⁡x→cf(x)\lim_{x\to c} f(x) exists; (3) lim⁡x→cf(x)=f(c)\lim_{x\to c} f(x) = f(c).
Evaluate the one-sided limit lim⁡x→2−∣x−2∣x−2\displaystyle\lim_{x\to 2^-} \frac{|x - 2|}{x - 2}.
When xx approaches 2 from the left (x<2x < 2), x−2<0x - 2 < 0, so ∣x−2∣=−(x−2)|x - 2| = -(x - 2). Substituting gives lim⁡x→2−−(x−2)x−2=lim⁡x→2−(−1)=−1\lim_{x\to 2^-} \frac{-(x - 2)}{x - 2} = \lim_{x\to 2^-} (-1) = -1. (Note: from the right, the limit is +1+1, so the two-sided limit does not exist).
📝 Chapter Quiz
2

Derivatives

The derivative is the first question of calculus made precise: the instantaneous rate of change of f f , equivalently the slope of the tangent line to its graph.

● Definition 2.1 — The derivative

The derivative of f f at x x is the limit of slopes of secant lines:

f′(x)=lim⁡h→0f(x+h)−f(x)h, f'(x)=\lim_{h\to 0}\frac{f(x+h)-f(x)}{h},

when this limit exists. It is also written dydx \dfrac{dy}{dx} or ddxf(x) \dfrac{d}{dx}f(x) .

As h→0 h\to 0 , the secant through (x,f(x)) \big(x,f(x)\big) and (x+h,f(x+h)) \big(x+h,f(x+h)\big) pivots into the tangent. Watch it happen — drag the point of tangency and the slope readout below updates live.

⊙ Explorer · Tangent line & slopeinteractive
height  f(a)—
slope  f′(a)—

The rules of differentiation

We rarely use the limit definition directly. These rules build every elementary derivative:

Power rule
ddxxn=n x n−1 \dfrac{d}{dx}x^{n}=n\,x^{\,n-1}
Constant multiple
ddx(c f)=c f′ \dfrac{d}{dx}\big(c\,f\big)=c\,f'
Sum
(f+g)′=f′+g′ (f+g)'=f'+g'
Product
(fg)′=f′g+fg′ (fg)'=f'g+fg'
Quotient
(fg)′=f′g−fg′g2 \Big(\dfrac{f}{g}\Big)'=\dfrac{f'g-fg'}{g^{2}}
Chain
ddxf(g(x))=f′ ⁣(g(x)) g′(x) \dfrac{d}{dx}f\big(g(x)\big)=f'\!\big(g(x)\big)\,g'(x)
▲ Reference — Common derivatives

ddxsin⁡x=cos⁡x \dfrac{d}{dx}\sin x=\cos x , ddxcos⁡x=−sin⁡x\quad \dfrac{d}{dx}\cos x=-\sin x , ddxtan⁡x=sec⁡2x\quad \dfrac{d}{dx}\tan x=\sec^2 x ,

ddxex=ex \dfrac{d}{dx}e^{x}=e^{x} , ddxln⁡x=1x(x>0).\quad \dfrac{d}{dx}\ln x=\dfrac1x \quad (x>0).

Worked example 2.A — Chain rule

Differentiate y=sin⁡ ⁣(3x2) y=\sin\!\big(3x^2\big) .

Outer function sin⁡u \sin u with u=3x2 u=3x^2 . Then dydu=cos⁡u \dfrac{dy}{du}=\cos u and dudx=6x \dfrac{du}{dx}=6x . By the chain rule,

dydx=cos⁡ ⁣(3x2)⋅6x=6xcos⁡ ⁣(3x2). \frac{dy}{dx}=\cos\!\big(3x^2\big)\cdot 6x = 6x\cos\!\big(3x^2\big).

Worked example 2.B — Product rule

Differentiate y=x2ex y=x^2 e^{x} .

With f=x2 f=x^2 (so f′=2x f'=2x ) and g=ex g=e^x (so g′=ex g'=e^x ):

y′=2x ex+x2ex=xex(x+2). y'=2x\,e^{x}+x^2 e^{x}=x e^{x}(x+2).

Coordinate plane with graph of y = x^2, Tangent: y = 2x - 1; marked points P(1, 1) (1, 1)-11224xyy = x²Tangent: y = 2x − 1P(1, 1)
Tangent line y=2x−1y = 2x - 1 to parabola y=x2y = x^2 at point of tangency P(1,1)P(1, 1), demonstrating gradient m=f′(1)=2m = f'(1) = 2.
⚠ Common Traps & Exam Pitfalls
Product Rule Trap: The derivative of a product is NOT the product of derivatives: (uv)′≠u′v′(uv)' \ne u'v'. Always use (uv)′=u′v+uv′(uv)' = u'v + uv'.

Quotient Rule Order: Order matters in subtraction: (uv)′=u′v−uv′v2\left(\frac{u}{v}\right)' = \frac{u'v - uv'}{v^2} (the numerator is u′v−uv′u'v - uv', never reversed).

Chain Rule Inner Function: When differentiating composite functions such as [g(x)]n[g(x)]^n, eg(x)e^{g(x)}, or sin⁡(g(x))\sin(g(x)), never forget to multiply by the derivative of the inside: g′(x)g'(x). For example, ddxcos⁡(5x)=−5sin⁡(5x)\frac{d}{dx}\cos(5x) = -5\sin(5x), not −sin⁡(5x)-\sin(5x).
Find the equation of the tangent line to the curve y=x3−4x+1y = x^3 - 4x + 1 at the point where x=2x = 2.
At x=2x = 2, y=23−4(2)+1=8−8+1=1y = 2^3 - 4(2) + 1 = 8 - 8 + 1 = 1, so the point is (2,1)(2, 1). Differentiating gives dydx=3x2−4\frac{dy}{dx} = 3x^2 - 4. At x=2x = 2, the slope is m=3(4)−4=8m = 3(4) - 4 = 8. Using point-slope form: y−1=8(x−2)  ⟹  y=8x−15y - 1 = 8(x - 2) \implies y = 8x - 15.
📝 Chapter Quiz
3

Integrals

The integral is the second question of calculus: how much accumulates. Geometrically, the definite integral measures the signed area between a curve and the horizontal axis.

● Definition 3.1 — Definite integral (as a limit of sums)

Partition [a,b] [a,b] into n n strips of width Δx=b−an \Delta x=\frac{b-a}{n} . Sampling a height in each strip and summing the rectangle areas gives a Riemann sum; the integral is its limit:

∫abf(x) dx=lim⁡n→∞∑i=1nf(xi∗) Δx. \int_a^b f(x)\,dx=\lim_{n\to\infty}\sum_{i=1}^{n} f(x_i^\ast)\,\Delta x.

The explorer below builds that limit by hand. Increase the number of rectangles and watch the approximation tighten onto the true area — the error column shrinks toward zero.

⊙ Explorer · Riemann sums → areainteractive
approx  Sₙ—
exact  ∫—
error—

Antiderivatives & the indefinite integral

Reversing differentiation, F F is an antiderivative of f f if F′=f F'=f . Since constants vanish under differentiation, antiderivatives carry a +C +C .

Power (n ≠ −1)
∫xn dx=xn+1n+1+C \displaystyle\int x^{n}\,dx=\frac{x^{n+1}}{n+1}+C
Reciprocal
∫1x dx=ln⁡∣x∣+C \displaystyle\int \frac{1}{x}\,dx=\ln|x|+C
Exponential
∫ex dx=ex+C \displaystyle\int e^{x}\,dx=e^{x}+C
Sine
∫sin⁡x dx=−cos⁡x+C \displaystyle\int \sin x\,dx=-\cos x+C
Cosine
∫cos⁡x dx=sin⁡x+C \displaystyle\int \cos x\,dx=\sin x+C
Linearity
∫(af+bg)=a ⁣∫ ⁣f+b ⁣∫ ⁣g \displaystyle\int (af+bg)=a\!\int\! f+b\!\int\! g
Worked example 3.A

Find the area under f(x)=x2 f(x)=x^2 from 0 0 to 2 2 .

An antiderivative is F(x)=x33 F(x)=\tfrac{x^3}{3} . Evaluating (using the Fundamental Theorem, next chapter):

∫02x2 dx=[x33]02=83−0=83≈2.667. \int_0^2 x^2\,dx=\Big[\tfrac{x^3}{3}\Big]_0^2=\tfrac{8}{3}-0=\tfrac{8}{3}\approx 2.667.

Coordinate plane with graph of y = x^2; marked points (0, 0) (0, 0), (2, 4) (2, 4)121234xyy = x²(0, 0)(2, 4)
Parabola y=x2y = x^2 over interval [0,2][0, 2] with shaded area representing the definite integral ∫02x2 dx=83\int_0^2 x^2\,dx = \frac{8}{3}.
⚠ Common Traps & Exam Pitfalls
Forgetting the Constant + C: Every indefinite integral represents an entire family of antiderivatives and MUST end with +C+ C. Missing +C+ C loses points on free-response exams.

Power Rule Exception for 1/x: The power rule ∫xn dx=xn+1n+1+C\int x^n\,dx = \frac{x^{n+1}}{n+1} + C is valid for all n≠−1n \ne -1. When n=−1n = -1, ∫1x dx=ln⁡∣x∣+C\int \frac{1}{x}\,dx = \ln|x| + C (with absolute value bars!).

Trigonometric Integral Signs: Reversing signs between differentiation and integration is very common: ∫sin⁡x dx=−cos⁡x+C\int \sin x\,dx = -\cos x + C (negative!), whereas ∫cos⁡x dx=+sin⁡x+C\int \cos x\,dx = +\sin x + C.

Non-Distributivity Over Products: You CANNOT integrate term-by-term across multiplication: ∫f(x)g(x) dx≠(∫f(x) dx)(∫g(x) dx)\int f(x)g(x)\,dx \ne \left(\int f(x)\,dx\right)\left(\int g(x)\,dx\right).
Evaluate the indefinite integral ∫(4x3−2x+3sin⁡x) dx\displaystyle\int \left(4x^3 - \frac{2}{x} + 3\sin x\right)\,dx.
Integrating term by term:
• ∫4x3 dx=x4\int 4x^3\,dx = x^4
• ∫−2x dx=−2ln⁡∣x∣\int -\frac{2}{x}\,dx = -2\ln|x|
• ∫3sin⁡x dx=−3cos⁡x\int 3\sin x\,dx = -3\cos x
Combining and adding the constant of integration yields: x4−2ln⁡∣x∣−3cos⁡x+Cx^4 - 2\ln|x| - 3\cos x + C.
📝 Chapter Quiz
4

The Fundamental Theorem

Here the two halves meet. The slope problem (indigo) and the area problem (amber) turn out to be inverses of one another — arguably the central result of all calculus.

▲ Theorem 4.1 — Fundamental Theorem of Calculus

Part I. If A(x)=∫axf(t) dt \displaystyle A(x)=\int_a^x f(t)\,dt , then A A is differentiable and A′(x)=f(x) A'(x)=f(x) . Differentiating an accumulated area recovers the original function.

Part II. If F F is any antiderivative of f f , then ∫abf(x) dx=F(b)−F(a). \displaystyle\int_a^b f(x)\,dx=F(b)-F(a). This is what makes integration computable.

The twin explorer makes Part I visible. The amber area on the upper graph is exactly the indigo height of the accumulation graph below. Drag x x : the rate at which the lower curve rises equals the upper curve's height at that instant — that is, A′(x)=f(x) A'(x)=f(x) .

⊙ Explorer · Accumulation A(x) = ∫ₐˣ finteractive
area  A(x)—
slope  A′(x)=f(x)—
Worked example 4.A — Putting it together

Evaluate ∫0πsin⁡x dx \displaystyle\int_0^{\pi} \sin x\,dx .

An antiderivative of sin⁡x \sin x is −cos⁡x -\cos x . By Part II,

∫0πsin⁡x dx=[−cos⁡x]0π=(−cos⁡π)−(−cos⁡0)=1+1=2. \int_0^{\pi}\sin x\,dx=\big[-\cos x\big]_0^{\pi}=(-\cos\pi)-(-\cos 0)=1+1=2.

▲ Fundamental Theorem of Calculus

Part I: If F(x)=∫axf(t) dt F(x)=\int_a^x f(t)\,dt , then F′(x)=f(x) F'(x)=f(x) .
Part II: ∫abf(x) dx=F(b)−F(a) \int_a^b f(x)\,dx = F(b)-F(a) where F′=f F'=f .

FTC Part I
ddx∫axf(t) dt=f(x) \dfrac{d}{dx}\int_a^x f(t)\,dt = f(x)
FTC Part II
∫abf(x) dx=F(b)−F(a) \int_a^b f(x)\,dx = F(b)-F(a)
Net change
∫abF′(x) dx=F(b)−F(a) \int_a^b F'(x)\,dx = F(b)-F(a)
Chain rule form
ddx∫ag(x) ⁣f(t) dt=f(g(x)) g′(x) \dfrac{d}{dx}\int_a^{g(x)}\!f(t)\,dt = f(g(x))\,g'(x)
Worked example

Evaluate ∫142x dx \int_1^4 2x\,dx .

F(x)=x2,F(4)−F(1)=16−1=15. F(x)=x^2,\quad F(4)-F(1)=16-1=15.

Worked example

Find ddx∫0x2cos⁡t dt \dfrac{d}{dx}\int_0^{x^2}\cos t\,dt .

cos⁡(x2)⋅2x=2xcos⁡(x2). \cos(x^2)\cdot 2x = 2x\cos(x^2).

Coordinate plane with graph of f(t) = cos(t), g(x) = sin(x); marked points g(0) = 0 (0, 0), Peak: g(π/2) = 1 (1.57, 1)123-11xyf(t) = cos(t)g(x) = sin(x)g(0) = 0Peak: g(π/2) = 1
Accumulation function g(x)=∫0xf(t) dtg(x) = \int_0^x f(t)\,dt measuring net area under f(t)f(t), illustrating the Fundamental Theorem of Calculus g′(x)=f(x)g'(x) = f(x).
⚠ Common Traps & Exam Pitfalls
FTC Part 1 Chain Rule Missing: When differentiating an integral with a variable upper limit u(x)u(x):
ddx∫au(x)f(t) dt=f(u(x))⋅u′(x) \frac{d}{dx}\int_a^{u(x)} f(t)\,dt = f(u(x)) \cdot u'(x)
Forgetting to multiply by u′(x)u'(x) is the single most penalized error in AP Calculus!

Lower Limit is a Function: If the variable is in the lower limit, reverse limits and negate first:
ddx∫u(x)bf(t) dt=−ddx∫bu(x)f(t) dt=−f(u(x))u′(x) \frac{d}{dx}\int_{u(x)}^b f(t)\,dt = -\frac{d}{dx}\int_b^{u(x)} f(t)\,dt = -f(u(x))u'(x)
Both Limits Variable: Split at a constant cc: ∫v(x)u(x)=∫cu(x)−∫cv(x)\int_{v(x)}^{u(x)} = \int_c^{u(x)} - \int_c^{v(x)}, yielding f(u(x))u′(x)−f(v(x))v′(x)f(u(x))u'(x) - f(v(x))v'(x).
Find the derivative h′(x)h'(x) for the accumulation function h(x)=∫2x31+t2 dth(x) = \displaystyle\int_2^{x^3} \sqrt{1 + t^2}\,dt.
By FTC Part 1 and the Chain Rule, let u=x3u = x^3 so that dudx=3x2\frac{du}{dx} = 3x^2. Then:
h′(x)=1+(x3)2⋅ddx(x3)=3x21+x6. h'(x) = \sqrt{1 + (x^3)^2} \cdot \frac{d}{dx}(x^3) = 3x^2 \sqrt{1 + x^6}.
📝 Chapter Quiz
5

Applications of Derivatives

The sign of the derivative tells us where a function rises or falls; the sign of the second derivative tells us how it bends. Together they locate maxima, minima, and inflection points — the heart of optimization.

● Definition 5.1 — Critical point

A critical point of f f is a value c c where f′(c)=0 f'(c)=0 or f′(c) f'(c) does not exist. Local maxima and minima can occur only at critical points.

▲ Theorem 5.2 — Monotonicity & concavity

On an interval: if f′>0 f'>0 then f f is increasing; if f′<0 f'<0 then f f is decreasing. If f′′>0 f''>0 the graph is concave up; if f′′<0 f''<0 it is concave down. An inflection point is where concavity changes.

Second derivative test. At a critical point c c : if f′′(c)>0 f''(c)>0 then c c is a local minimum; if f′′(c)<0 f''(c)<0 then c c is a local maximum.

Optimization puts this to work: model the quantity, differentiate, set the derivative to zero, and confirm the extremum. The explorer animates the classic box problem — the volume rises to a single peak exactly where V′(x)=0 V'(x)=0 .

⊙ Explorer · Optimizing an open boxinteractive
volume  V(x)—
maximum—

Cut squares of side xx from a 10×810\times 8 sheet and fold up: V(x)=x(10−2x)(8−2x)V(x)=x(10-2x)(8-2x). The amber marker is the maximum.

Worked example 5.A — Local extrema

Find and classify the extrema of f(x)=x3−3x f(x)=x^3-3x .

Critical points: f′(x)=3x2−3=3(x−1)(x+1)=0⇒x=±1 f'(x)=3x^2-3=3(x-1)(x+1)=0 \Rightarrow x=\pm 1 . Use f′′(x)=6x f''(x)=6x :

f′′(1)=6>0 (min),f′′(−1)=−6<0 (max). f''(1)=6>0 \ (\text{min}),\qquad f''(-1)=-6<0 \ (\text{max}).

So a local minimum at (1,−2) (1,-2) and a local maximum at (−1,2) (-1,2) .

Worked example 5.B — Optimization

A rectangular pen is built against a wall using 100 100 m of fence on the other three sides. Maximise the area.

Let the two perpendicular sides be x x ; the parallel side is 100−2x 100-2x . Then A(x)=x(100−2x)=100x−2x2 A(x)=x(100-2x)=100x-2x^2 , so A′(x)=100−4x=0⇒x=25 A'(x)=100-4x=0 \Rightarrow x=25 .

Dimensions 25×50,Amax⁡=1250 m2. \text{Dimensions } 25\times 50, \qquad A_{\max}=1250\ \text{m}^2.

Related rates

When two quantities are tied together by an equation and both vary with time, differentiate the relation with respect to t t (chain rule) to connect their rates.

Worked example 5.C — Related rates

A spherical balloon is inflated so its radius grows at drdt=2 \dfrac{dr}{dt}=2 cm/s. How fast is the volume increasing when r=5 r=5 cm?

From V=43πr3 V=\tfrac{4}{3}\pi r^3 , differentiate with respect to t t : dVdt=4πr2drdt \dfrac{dV}{dt}=4\pi r^2\dfrac{dr}{dt} . At r=5 r=5 :

dVdt=4π(25)(2)=200π cm3/s. \frac{dV}{dt}=4\pi(25)(2)=200\pi\ \text{cm}^3/\text{s}.

L'Hôpital's Rule

▲ Theorem 5.3 — L'Hôpital's Rule

If lim⁡x→af(x)g(x) \displaystyle\lim_{x\to a}\dfrac{f(x)}{g(x)} has indeterminate form 00 \tfrac00 or ∞∞ \tfrac{\infty}{\infty} , then

lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x), \lim_{x\to a}\frac{f(x)}{g(x)}=\lim_{x\to a}\frac{f'(x)}{g'(x)},

provided the right-hand limit exists.

Worked example 5.D — L'Hôpital

Evaluate lim⁡x→∞ln⁡xx \displaystyle\lim_{x\to\infty}\frac{\ln x}{x} (form ∞∞ \tfrac{\infty}{\infty} ).

Differentiate top and bottom: ddxln⁡x=1x \dfrac{d}{dx}\ln x=\tfrac1x , ddxx=1 \dfrac{d}{dx}x=1 :

lim⁡x→∞ln⁡xx=lim⁡x→∞1/x1=0. \lim_{x\to\infty}\frac{\ln x}{x}=\lim_{x\to\infty}\frac{1/x}{1}=0.

▲ Key derivative applications

Derivatives measure rates of change. The first derivative test locates local extrema; the second derivative test distinguishes minima from maxima and reveals concavity.

Critical point
f′(c)=0 f'(c)=0 or f′(c) f'(c) undefined
1st deriv. test
f′ f' changes +→− +\to- : local max; −→+ -\to+ : local min
2nd deriv. test
f′′(c)>0 f''(c)>0 : min; f′′(c)<0 f''(c)<0 : max
L'Hôpital
lim⁡fg ⁣= ⁣lim⁡f′g′ \lim\dfrac{f}{g}\!=\!\lim\dfrac{f'}{g'} when 00 \tfrac{0}{0} or ∞∞ \tfrac{\infty}{\infty}
Worked example — optimization

A farmer has 200 m of fencing to enclose a rectangle against a wall. Find dimensions maximizing area.

Let width =x = x , length =200−2x = 200-2x . Area A=x(200−2x)=200x−2x2 A=x(200-2x)=200x-2x^2 .

A′=200−4x=0  ⟹  x=50 m,  L=100 m. A'=200-4x=0 \implies x=50\text{ m},\; L=100\text{ m}.

Worked example — related rates

A ladder 10 m long slides down a wall. When the base is 6 m from the wall and moving out at 2 m/s, how fast is the top falling?

x2+y2=100  ⟹  2xdxdt+2ydydt=0. x^2+y^2=100 \implies 2x\tfrac{dx}{dt}+2y\tfrac{dy}{dt}=0.

At x=6 x=6 , y=8 y=8 : 12(2)+16dydt=0⇒dydt=−1.5 12(2)+16\dfrac{dy}{dt}=0 \Rightarrow \dfrac{dy}{dt}=-1.5 m/s.

Coordinate plane with graph of f(x) = x^3 - 3x; marked points Local Max (-1, 2) (-1, 2), Local Min (1, -2) (1, -2)-2-112-22xyf(x) = x³ − 3xLocal Max (-1, 2)Local Min (1, -2)
Cubic polynomial f(x)=x3−3xf(x) = x^3 - 3x exhibiting local maximum at (−1,2)(-1, 2) and local minimum at (1,−2)(1, -2), where f′(x)=0f'(x) = 0.
⚠ Common Traps & Exam Pitfalls
Critical Points vs Extrema: A critical point f′(c)=0f'(c) = 0 or undefined is a candidate, NOT a guarantee of an extremum. For example, f(x)=x3f(x) = x^3 has f′(0)=0f'(0) = 0, but changes sign neither way — it is an inflection point, not a max or min!

Absolute Extrema on Closed Intervals: By the Extreme Value Theorem, continuous ff on [a,b][a, b] attains an absolute max and min. You MUST evaluate candidates at critical points AND at both endpoints f(a)f(a) and f(b)f(b).

Related Rates Premature Substitution: Differentiate your geometric relation implicitly with respect to tt FIRST. Never substitute instantaneous values (e.g. x=6x = 6) before differentiating, or the derivative will erroneously treat variables as constants!
Find the absolute maximum and minimum values of f(x)=2x3−3x2−12x+5f(x) = 2x^3 - 3x^2 - 12x + 5 on the closed interval [0,3][0, 3].
Find critical points: f′(x)=6x2−6x−12=6(x2−x−2)=6(x−2)(x+1)=0f'(x) = 6x^2 - 6x - 12 = 6(x^2 - x - 2) = 6(x - 2)(x + 1) = 0. The roots are x=2x = 2 and x=−1x = -1. Only x=2x = 2 lies in [0,3][0, 3].
Evaluate at endpoints and interior critical point:
• f(0)=5f(0) = 5
• f(2)=2(8)−3(4)−12(2)+5=16−12−24+5=−15f(2) = 2(8) - 3(4) - 12(2) + 5 = 16 - 12 - 24 + 5 = -15
• f(3)=2(27)−3(9)−12(3)+5=54−27−36+5=−4f(3) = 2(27) - 3(9) - 12(3) + 5 = 54 - 27 - 36 + 5 = -4
Absolute maximum is 55 (at x=0x = 0); Absolute minimum is −15-15 (at x=2x = 2).
📝 Chapter Quiz
6

Techniques of Integration

Most integrals are not in a table. Two techniques reverse the differentiation rules you already know and unlock the majority of exam problems.

▲ Theorem 6.1 — Substitution (reverse chain rule)

If u=g(x) u=g(x) then du=g′(x) dx du=g'(x)\,dx , and

∫f(g(x)) g′(x) dx=∫f(u) du. \int f\big(g(x)\big)\,g'(x)\,dx=\int f(u)\,du.

Choose u u so that its derivative also appears (up to a constant) in the integrand.

▲ Theorem 6.2 — Integration by parts

From the product rule, ∫u dv=uv−∫v du. \displaystyle\int u\,dv = uv-\int v\,du. Pick u u by LIATE (logarithms, inverse-trig, algebraic, trig, exponential — earlier letters make better u u ).

Worked example 6.A — Substitution

Evaluate ∫2xcos⁡ ⁣(x2) dx \displaystyle\int 2x\cos\!\big(x^2\big)\,dx .

Let u=x2 u=x^2 , so du=2x dx du=2x\,dx . The integral becomes ∫cos⁡u du \int \cos u\,du :

∫2xcos⁡ ⁣(x2) dx=sin⁡ ⁣(x2)+C. \int 2x\cos\!\big(x^2\big)\,dx=\sin\!\big(x^2\big)+C.

Worked example 6.B — By parts

Evaluate ∫x ex dx \displaystyle\int x\,e^{x}\,dx .

Let u=x, dv=exdx u=x,\ dv=e^{x}dx , so du=dx, v=ex du=dx,\ v=e^{x} . Then uv−∫v du uv-\int v\,du :

∫x ex dx=xex−∫ex dx=ex(x−1)+C. \int x\,e^{x}\,dx=x e^{x}-\int e^{x}\,dx=e^{x}(x-1)+C.

▲ Integration techniques

Beyond basic antiderivatives: substitution reverses the chain rule; integration by parts reverses the product rule; partial fractions decompose rational integrands.

Substitution
∫f(g(x))g′(x) dx=F(g(x))+C \int f(g(x))g'(x)\,dx = F(g(x))+C
By parts
∫u dv=uv−∫v du \int u\,dv = uv - \int v\,du
Trig sub
a2−x2 \sqrt{a^2-x^2}: set x=asin⁡θ x=a\sin\theta
Partial fractions
1(x−a)(x−b)=Ax−a+Bx−b \dfrac{1}{(x-a)(x-b)}=\dfrac{A}{x-a}+\dfrac{B}{x-b}
Worked example — substitution

Evaluate ∫2xex2 dx \int 2x e^{x^2}\,dx .

Let u=x2 u=x^2 , du=2x dx du=2x\,dx : ∫eu du=ex2+C \int e^u\,du = e^{x^2}+C .

Worked example — by parts

Evaluate ∫xcos⁡x dx \int x\cos x\,dx .

Let u=x u=x , dv=cos⁡x dx dv=\cos x\,dx . Then du=dx du=dx , v=sin⁡x v=\sin x :

xsin⁡x−∫sin⁡x dx=xsin⁡x+cos⁡x+C. x\sin x - \int\sin x\,dx = x\sin x + \cos x + C.

Coordinate plane with graph of f(x) = x e^{-x}; marked points (0, 0) (0, 0), Peak (1, 1/e) (1, 0.368)123xyf(x) = x e^{-x}(0, 0)Peak (1, 1/e)
Graph of integrand f(x)=xe−xf(x) = x e^{-x}, highlighting the weighting factor in integration by parts ∫xe−x dx\int x e^{-x}\,dx.
⚠ Common Traps & Exam Pitfalls
Integration by Parts Sign Error: The formula is ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du. Forgetting that the second term has a MINUS sign (or mishandling double negatives when vv is negative) is a chronic trap.

Choosing u via LIATE: Prioritize uu in the order: Logarithmic, Inverse trig, Algebraic, Trigonometric, Exponential. Differentiating uu must simplify the remaining integrand.

Partial Fractions Improper Rational Functions: The method of partial fractions ONLY applies when the numerator degree is strictly LESS than the denominator degree. If deg⁡(P)≥deg⁡(Q)\deg(P) \ge \deg(Q), you MUST perform polynomial long division first!

Definite Integrals with U-Sub: Remember to update limits of integration: x=a→u(a)x = a \to u(a), x=b→u(b)x = b \to u(b). Evaluating using original limits on a uu-expression is an automatic deduction.
Evaluate the indefinite integral ∫xe2x dx\displaystyle\int x e^{2x}\,dx using integration by parts.
Let u=xu = x and dv=e2x dxdv = e^{2x}\,dx. Then du=dxdu = dx and v=12e2xv = \frac{1}{2}e^{2x}.
Applying ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du:
∫xe2x dx=12xe2x−∫12e2x dx=12xe2x−14e2x+C=14e2x(2x−1)+C. \int x e^{2x}\,dx = \frac{1}{2}x e^{2x} - \int \frac{1}{2}e^{2x}\,dx = \frac{1}{2}x e^{2x} - \frac{1}{4}e^{2x} + C = \frac{1}{4}e^{2x}(2x - 1) + C.
📝 Chapter Quiz
7

Applications of Integration

Definite integrals measure accumulated quantities: the area trapped between two curves, the volume swept out by rotating a region, or the average height of a function.

▲ Theorem 7.1 — Area, volume, average

Area between curves: A=∫ab[ f(x)−g(x) ] dx \displaystyle A=\int_a^b \big[\,f(x)-g(x)\,\big]\,dx where f f is the upper curve.

Volume of revolution (disks): V=π∫ab[R(x)]2 dx. \displaystyle V=\pi\int_a^b \big[R(x)\big]^2\,dx.

Average value: fˉ=1b−a∫abf(x) dx. \displaystyle \bar f=\frac{1}{b-a}\int_a^b f(x)\,dx.

Drag the line in the explorer: the amber region is the area enclosed between the parabola and the line, recomputed live between their intersection points.

⊙ Explorer · Area between two curvesinteractive
y = 4 − x²  and  y = x + 2
intersection—
enclosed area—
Worked example 7.A — Area between curves

Find the area between y=x y=x and y=x2 y=x^2 on [0,1] [0,1] .

Here x≥x2 x\geq x^2 on [0,1] [0,1] , so integrate the difference:

∫01(x−x2) dx=[x22−x33]01=12−13=16. \int_0^1 \big(x-x^2\big)\,dx=\Big[\tfrac{x^2}{2}-\tfrac{x^3}{3}\Big]_0^1=\tfrac12-\tfrac13=\tfrac16.

Worked example 7.B — Volume of revolution

The region under y=x y=\sqrt{x} on [0,4] [0,4] is revolved about the x x -axis. Find the volume.

Disk method with R(x)=x R(x)=\sqrt{x} , so R2=x R^2=x :

V=π∫04x dx=π[x22]04=8π. V=\pi\int_0^4 x\,dx=\pi\Big[\tfrac{x^2}{2}\Big]_0^4=8\pi.

▲ Geometric and physical applications

Definite integrals compute areas between curves, volumes of solids of revolution, arc lengths, and work done by variable forces.

Area between curves
∫ab[f(x)−g(x)] dx \int_a^b[f(x)-g(x)]\,dx
Disk method
V=π∫ab[f(x)]2 dx V=\pi\int_a^b[f(x)]^2\,dx
Shell method
V=2π∫abx f(x) dx V=2\pi\int_a^b x\,f(x)\,dx
Arc length
L=∫ab1+[f′(x)]2 dx L=\int_a^b\sqrt{1+[f'(x)]^2}\,dx
Worked example — area

Find the area between y=x2 y=x^2 and y=x y=x from x=0 x=0 to x=1 x=1 .

∫01(x−x2) dx=[x22−x33]01=16. \int_0^1(x-x^2)\,dx = \left[\frac{x^2}{2}-\frac{x^3}{3}\right]_0^1 = \frac{1}{6}.

Worked example — disk volume

Find the volume when y=x y=\sqrt{x} on [0,4] [0,4] is revolved about the x x -axis.

V=π∫04x dx=π⋅8=8π. V=\pi\int_0^4 x\,dx = \pi\cdot 8 = 8\pi.

Coordinate plane with graph of y = x (top), y = x^2 (bottom); marked points (0, 0) (0, 0), (1, 1) (1, 1)11xyy = x (top)y = x² (bottom)(0, 0)(1, 1)
Region bounded between curves y=xy = x and y=x2y = x^2 on [0,1][0, 1], where upper curve minus lower curve gives area A=16A = \frac{1}{6}.
⚠ Common Traps & Exam Pitfalls
Top Minus Bottom Rule: When finding area between curves, always integrate ∫ab[ytop−ybottom] dx\int_a^b [y_{\text{top}} - y_{\text{bottom}}]\,dx. If the curves intersect within the interval, you MUST split the integral at intersection points, or positive and negative areas will cancel each other out!

Washer Method Error: The washer formula for volume of revolution is V=π∫[R(x)2−r(x)2] dxV = \pi \int [R(x)^2 - r(x)^2]\,dx. It is NEVER π∫[R(x)−r(x)]2 dx\pi \int [R(x) - r(x)]^2\,dx (squaring the difference is wrong!).

Off-Axis Revolutions: When revolving around y=ky = k instead of the xx-axis, the radius is the distance to the axis of revolution: R(x)=∣f(x)−k∣R(x) = |f(x) - k|.
Find the volume of the solid generated when the region bounded by y=x2y = x^2, y=0y = 0, and x=2x = 2 is revolved about the xx-axis.
Using the disk method with R(x)=x2R(x) = x^2:
V=π∫02[R(x)]2 dx=π∫02x4 dx=π[x55]02=π(325−0)=32π5. V = \pi \int_0^2 [R(x)]^2\,dx = \pi \int_0^2 x^4\,dx = \pi \left[\frac{x^5}{5}\right]_0^2 = \pi \left(\frac{32}{5} - 0\right) = \frac{32\pi}{5}.
📝 Chapter Quiz
8

Differential Equations

A differential equation relates a function to its own rate of change. Solving one means finding every function whose derivative behaves as prescribed — the language in which growth, cooling, and motion are written.

● Definition 8.1 — Differential equation

An equation involving an unknown function and its derivatives, such as dydx=f(x,y) \dfrac{dy}{dx}=f(x,y) . A solution is a function y(x) y(x) that satisfies it; an initial condition picks out one particular solution.

Separable equations. If dydx=g(x) h(y) \dfrac{dy}{dx}=g(x)\,h(y) , gather each variable on its own side and integrate:

∫dyh(y)=∫g(x) dx. \int \frac{dy}{h(y)}=\int g(x)\,dx.

▲ Theorem 8.2 — Exponential model

The equation dydt=ky \dfrac{dy}{dt}=ky has solution y=y0 ekt y=y_0\,e^{kt} : exponential growth when k>0 k>0 and decay when k<0 k<0 .

A slope field draws the prescribed slope at a grid of points; solution curves simply flow along it. Pick an equation and slide the initial value — the amber curve threads through the field from (0, y0) (0,\,y_0) .

⊙ Explorer · Slope field & solution curveinteractive
equationdy/dx = y
solution through (0, y₀)—
Worked example 8.A — Separable

Solve dydx=2xy \dfrac{dy}{dx}=2xy .

Separate and integrate: ∫dyy=∫2x dx \displaystyle\int\frac{dy}{y}=\int 2x\,dx , so ln⁡∣y∣=x2+C \ln|y|=x^2+C . Exponentiating,

y=Ce x2. y=C e^{\,x^2}.

Worked example 8.B — Initial value problem

Solve dydx=3y \dfrac{dy}{dx}=3y with y(0)=4 y(0)=4 .

By the exponential model y=y0ekt y=y_0 e^{kt} with k=3 k=3 , and y(0)=4 y(0)=4 :

y=4e3x. y=4e^{3x}.

▲ Ordinary differential equations

A differential equation relates a function to its derivatives. Separable ODEs are solved by separating variables and integrating both sides.

Separable ODE
dydx=g(x)h(y)⇒∫dyh(y)=∫g(x) dx \dfrac{dy}{dx}=g(x)h(y) \Rightarrow \int\dfrac{dy}{h(y)}=\int g(x)\,dx
Exponential growth
y′=ky⇒y=y0ekt y'=ky \Rightarrow y=y_0 e^{kt}
Integrating factor
y′+P(x)y=Q(x) y'+P(x)y=Q(x) , μ=e∫P dx \mu=e^{\int P\,dx}
Logistic model
dPdt=kP ⁣(1−PM) \dfrac{dP}{dt}=kP\!\left(1-\dfrac{P}{M}\right)
Worked example

Solve dydx=2xy \dfrac{dy}{dx}=2xy , y(0)=3 y(0)=3 .

∫dyy=∫2x dx  ⟹  ln⁡∣y∣=x2+C  ⟹  y=3ex2. \int\frac{dy}{y}=\int 2x\,dx \implies \ln|y|=x^2+C \implies y=3e^{x^2}.

Slope field for differential equation dy/dx = x - y: dy/dx = x - ydy/dx = x - y
Slope field for first-order differential equation dydx=x−y\frac{dy}{dx} = x - y with particular solution curve passing through (0,1)(0, 1).
⚠ Common Traps & Exam Pitfalls
Separation of Variables Rules: Variables must separate completely into g(y) dy=f(x) dxg(y)\,dy = f(x)\,dx. Equations with sums like dydx=x+y\frac{dy}{dx} = x + y CANNOT be separated by subtraction! Treat dydy and dxdx as algebraic differentials in numerators.

Position of the Constant + C: The constant CC MUST be introduced at the exact moment of integration: ln⁡∣y∣=kx+C\ln|y| = kx + C. Exponentiating gives ∣y∣=ekx+C=eCekx=Aekx|y| = e^{kx+C} = e^C e^{kx} = A e^{kx}. Adding +C+ C at the end to get y=ekx+Cy = e^{kx} + C is a fatal algebraic error.

Slope Field Zero Slopes: Points where dydx=0\frac{dy}{dx} = 0 produce horizontal tick marks. Points where the derivative is undefined (e.g. division by zero) produce no tick marks or vertical asymptotes.
Find the particular solution to dydx=3x2y\dfrac{dy}{dx} = \dfrac{3x^2}{y} given the initial condition y(0)=4y(0) = 4.
Separate variables: y dy=3x2 dxy\,dy = 3x^2\,dx.
Integrate both sides: ∫y dy=∫3x2 dx  ⟹  12y2=x3+C\int y\,dy = \int 3x^2\,dx \implies \frac{1}{2}y^2 = x^3 + C.
Apply initial condition y(0)=4y(0) = 4: 12(4)2=03+C  ⟹  8=C\frac{1}{2}(4)^2 = 0^3 + C \implies 8 = C.
Hence, 12y2=x3+8  ⟹  y2=2x3+16\frac{1}{2}y^2 = x^3 + 8 \implies y^2 = 2x^3 + 16. Since y(0)=4>0y(0) = 4 > 0, we take the positive root: y=2x3+16y = \sqrt{2x^3 + 16}.
📝 Chapter Quiz
9

Parametric & Polar

Not every curve is a function y=f(x) y=f(x) . Parametric equations trace a path through time, and polar coordinates describe position by distance and angle — both unlock curves that loop, spiral, and cross themselves.

▲ Theorem 9.1 — Parametric calculus

For a curve (x(t), y(t)) \big(x(t),\,y(t)\big) , the slope and arc length are

dydx=dy/dtdx/dt,L=∫ab(dxdt)2+(dydt)2  dt. \frac{dy}{dx}=\frac{dy/dt}{dx/dt},\qquad L=\int_a^b\sqrt{\Big(\tfrac{dx}{dt}\Big)^2+\Big(\tfrac{dy}{dt}\Big)^2}\;dt.

▲ Theorem 9.2 — Polar coordinates & area

With x=rcos⁡θ, y=rsin⁡θ x=r\cos\theta,\ y=r\sin\theta , the area swept by a polar curve is

A=12∫αβr2 dθ. A=\frac12\int_\alpha^\beta r^2\,d\theta.

Drag the trace slider to watch each curve drawn by its parameter — the indigo portion is traced so far, the amber dot is the current point.

⊙ Explorer · Tracing parametric & polar curvesinteractive
current point—
Worked example 9.A — Parametric slope

For x=t3, y=t2 x=t^3,\ y=t^2 , find dydx \dfrac{dy}{dx} .

Differentiate each: dxdt=3t2 \dfrac{dx}{dt}=3t^2 , dydt=2t \dfrac{dy}{dt}=2t . Then

dydx=2t3t2=23t. \frac{dy}{dx}=\frac{2t}{3t^2}=\frac{2}{3t}.

Worked example 9.B — Polar area

Find the area enclosed by the cardioid r=1+cos⁡θ r=1+\cos\theta .

Apply A=12∫02πr2 dθ A=\tfrac12\int_0^{2\pi} r^2\,d\theta with r2=1+2cos⁡θ+cos⁡2θ r^2=1+2\cos\theta+\cos^2\theta :

A=12∫02π(1+2cos⁡θ+cos⁡2θ) dθ=3π2. A=\frac12\int_0^{2\pi}\big(1+2\cos\theta+\cos^2\theta\big)\,d\theta=\frac{3\pi}{2}.

▲ Parametric and polar calculus

Parametric curves express x x and y y in terms of a parameter t t . Polar coordinates use (r,θ) (r,\theta) . Both require adapted formulas for slopes, arc lengths, and areas.

Parametric slope
dydx=dy/dtdx/dt \dfrac{dy}{dx}=\dfrac{dy/dt}{dx/dt}
Parametric arc length
L=∫ab(dxdt)2+(dydt)2 dt L=\int_a^b\sqrt{\left(\frac{dx}{dt}\right)^2+\left(\frac{dy}{dt}\right)^2}\,dt
Polar area
A=12∫αβr2 dθ A=\dfrac{1}{2}\int_\alpha^\beta r^2\,d\theta
Polar to rect.
x=rcos⁡θ,  y=rsin⁡θ x=r\cos\theta,\; y=r\sin\theta
Worked example

Find dydx \dfrac{dy}{dx} for x=t2 x=t^2 , y=t3 y=t^3 .

dydx=3t22t=3t2. \frac{dy}{dx}=\frac{3t^2}{2t}=\frac{3t}{2}.

Worked example — polar area

Area enclosed by r=2cos⁡θ r=2\cos\theta , a circle of radius 1:

A=12∫−π/2π/24cos⁡2θ dθ=π. A=\frac{1}{2}\int_{-\pi/2}^{\pi/2}4\cos^2\theta\,d\theta = \pi.

Unit circle diagram showing terminal angle 45: Trigonometric and Polar Coordinates ReferenceTrigonometric and Polar Coordinates Referencexy45°(0.707, 0.707)
Unit circle reference with terminal point (cos⁡θ,sin⁡θ)(\cos\theta, \sin\theta) and angle θ=45°\theta = 45° (π4\frac{\pi}{4} rad).
⚠ Common Traps & Exam Pitfalls
Second Derivative in Parametric: The second derivative is d2ydx2=ddt(dy/dx)dx/dt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(dy/dx)}{dx/dt}. It is NEVER the quotient of second derivatives d2y/dt2d2x/dt2\frac{d^2y/dt^2}{d^2x/dt^2}! You must differentiate the first derivative with respect to tt and divide again by dxdt\frac{dx}{dt}.

Missing 1/2 in Polar Area: Polar area is A=12∫αβr2 dθA = \frac{1}{2} \int_\alpha^\beta r^2\,d\theta. Forgetting the factor of 12\frac{1}{2} is the most frequent blunder on polar questions.

Polar Slope vs dr/dθ: In polar coordinates, drdθ\frac{dr}{d\theta} is the rate of change of radius with angle, NOT the slope of the curve! To find tangent slope dydx\frac{dy}{dx}, convert via x=rcos⁡θx = r\cos\theta, y=rsin⁡θy = r\sin\theta and calculate dy/dθdx/dθ\frac{dy/d\theta}{dx/d\theta}.
A particle moves along a curve defined parametrically by x=t2+1x = t^2 + 1 and y=t3−3ty = t^3 - 3t. Find the value of d2ydx2\dfrac{d^2y}{dx^2} at t=2t = 2.
First find the components: dxdt=2t\frac{dx}{dt} = 2t and dydt=3t2−3\frac{dy}{dt} = 3t^2 - 3.
The first derivative is dydx=3t2−32t=32t−32t\frac{dy}{dx} = \frac{3t^2 - 3}{2t} = \frac{3}{2}t - \frac{3}{2t}.
Differentiating with respect to tt: ddt(dydx)=32+32t2\frac{d}{dt}\left(\frac{dy}{dx}\right) = \frac{3}{2} + \frac{3}{2t^2}.
Then d2ydx2=ddt(dy/dx)dx/dt=32+32t22t\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(dy/dx)}{dx/dt} = \frac{\frac{3}{2} + \frac{3}{2t^2}}{2t}.
At t=2t = 2: numerator is 32+38=158\frac{3}{2} + \frac{3}{8} = \frac{15}{8}; denominator is 2(2)=42(2) = 4.
Thus d2ydx2=15/84=1532\frac{d^2y}{dx^2} = \frac{15/8}{4} = \frac{15}{32}.
📝 Chapter Quiz
10

Sequences & Series

A series adds infinitely many terms. Remarkably, many familiar functions can be written as “infinite polynomials” — and a short stretch of that polynomial already approximates the function beautifully near a point.

● Definition 10.1 — Series & convergence

An infinite series ∑n=1∞an \sum_{n=1}^{\infty} a_n converges if its partial sums SN=∑n=1Nan S_N=\sum_{n=1}^{N} a_n approach a finite limit as N→∞ N\to\infty ; otherwise it diverges.

▲ Theorem 10.2 — Geometric series

For ∣r∣<1 |r|<1 , the geometric series converges:

∑n=0∞a rn=a1−r. \sum_{n=0}^{\infty} a\,r^{n}=\frac{a}{1-r}.

If ∣r∣≥1 |r|\geq 1 it diverges. The p p -series ∑1/np \sum 1/n^{p} converges exactly when p>1 p>1 .

▲ Theorem 10.3 — Taylor & Maclaurin series

Near x=0 x=0 , a smooth function equals its Maclaurin series f(x)=∑n=0∞f(n)(0)n!xn \displaystyle f(x)=\sum_{n=0}^{\infty}\frac{f^{(n)}(0)}{n!}x^{n} . Three to know:

ex=∑xnn!,sin⁡x=∑(−1)nx2n+1(2n+1)!,cos⁡x=∑(−1)nx2n(2n)!. e^{x}=\sum \frac{x^{n}}{n!},\quad \sin x=\sum \frac{(-1)^{n}x^{2n+1}}{(2n+1)!},\quad \cos x=\sum \frac{(-1)^{n}x^{2n}}{(2n)!}.

The explorer builds the Maclaurin polynomial for sin⁡x \sin x one term at a time. With a single term it is just the line y=x y=x ; add more and the amber curve wraps itself around sin⁡x \sin x across an ever-wider interval.

⊙ Explorer · Taylor polynomials of sin xinteractive
functionsin x
approximationdegree 3

NN nonzero terms match sin⁡x\sin x through degree 2N−12N-1. Far from 00 the polynomial eventually peels away.

Geometric series
∑n=0∞arn=a1−r,  ∣r∣<1 \displaystyle\sum_{n=0}^\infty ar^n=\frac{a}{1-r},\;|r|<1
p-series test
∑1np \sum\frac{1}{n^p} converges iff p>1 p>1
Ratio test
L=lim⁡∣an+1an∣ L=\lim\left|\frac{a_{n+1}}{a_n}\right| ; converges if L<1 L<1 , diverges if L>1 L>1
Alternating series
Converges if bn↘0 b_n\searrow 0 monotonically
Worked example 10.A — Infinite geometric series

Evaluate ∑n=0∞(12)n \displaystyle\sum_{n=0}^{\infty}\Big(\tfrac{1}{2}\Big)^{n} .

Here a=1, r=12 a=1,\ r=\tfrac12 , and ∣r∣<1 |r|<1 , so the series converges:

a1−r=11−12=2. \frac{a}{1-r}=\frac{1}{1-\tfrac12}=2.

Worked example 10.B — Maclaurin approximation

Approximate e0.1 e^{0.1} with a third-degree Taylor polynomial.

Using ex≈1+x+x22+x36 e^{x}\approx 1+x+\tfrac{x^2}{2}+\tfrac{x^3}{6} at x=0.1 x=0.1 :

1+0.1+0.005+0.000167≈1.1052. 1+0.1+0.005+0.000167\approx 1.1052.

Coordinate plane with graph of sin(x), T1(x) = x, T3(x) = x - x^3/6; marked points Center (0, 0) (0, 0)-3-2-1123-11xysin(x)T1(x) = xT3(x) = x − x³/6Center (0, 0)
Taylor polynomial approximations of sin⁡x\sin x: linear T1(x)=xT_1(x) = x, cubic T3(x)=x−x36T_3(x) = x - \frac{x^3}{6}, and quintic T5(x)=x−x36+x5120T_5(x) = x - \frac{x^3}{6} + \frac{x^5}{120}.
⚠ Common Traps & Exam Pitfalls
The Divergence Test Fallacy: If lim⁡n→∞an=0\lim_{n\to\infty} a_n = 0, the series MAY converge or diverge. For example, the harmonic series ∑1n\sum \frac{1}{n} diverges even though its terms shrink to zero! The nth-term test can ONLY establish divergence (when lim⁡an≠0\lim a_n \ne 0), never convergence.

Taylor Series Center: If a Taylor series is centered at x=ax = a, every term must be a power of (x−a)(x - a), not xx: Pn(x)=∑k=0nf(k)(a)k!(x−a)kP_n(x) = \sum_{k=0}^n \frac{f^{(k)}(a)}{k!}(x - a)^k.

Alternating Series Remainder Bound: For an alternating series satisfying Leibniz's conditions, the error in approximating the infinite sum by the NN-th partial sum is strictly bounded by the absolute value of the first omitted term: ∣S−SN∣≤aN+1|S - S_N| \le a_{N+1}.
Find the third-degree Maclaurin polynomial P3(x)P_3(x) for f(x)=cos⁡xf(x) = \cos x.
Compute derivatives at x=0x = 0:
• f(0)=cos⁡(0)=1f(0) = \cos(0) = 1
• f′(0)=−sin⁡(0)=0f'(0) = -\sin(0) = 0
• f′′(0)=−cos⁡(0)=−1f''(0) = -\cos(0) = -1
• f′′′(0)=sin⁡(0)=0f'''(0) = \sin(0) = 0
Applying the Maclaurin formula: P3(x)=f(0)+f′(0)x+f′′(0)2!x2+f′′′(0)3!x3=1−x22P_3(x) = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3 = 1 - \frac{x^2}{2}. (Notice the cubic term has coefficient 0).
📝 Chapter Quiz
11

Convergence Tests & Power Series

A series ∑an \sum a_n converges when its partial sums SN=∑n=1Nan S_N=\sum_{n=1}^{N}a_n approach a finite limit. Since we rarely sum infinitely many terms by hand, a battery of tests decides convergence from the shape of an a_n alone.

▲ Theorem 11.1 — The nth-term test

If lim⁡n→∞an≠0 \displaystyle\lim_{n\to\infty}a_n\neq 0 , then ∑an \sum a_n diverges. Caution: an→0 a_n\to 0 does not guarantee convergence — the harmonic series ∑1n \sum \tfrac1n diverges even though its terms vanish.

▲ Theorem 11.2 — p-series & comparison

The p-series ∑n=1∞1np \displaystyle\sum_{n=1}^{\infty}\frac{1}{n^{p}} converges if and only if p>1 p\gt 1 . For positive terms, if 0≤an≤bn 0\le a_n\le b_n and ∑bn \sum b_n converges, so does ∑an \sum a_n (and the contrapositive for divergence).

⊙ Explorer · Partial sums approaching a limitinteractive
partial sum SN0.9844
limit1.0000
remainder0.0156

The geometric series ∑(12)n\sum (\tfrac12)^n sums to 11. Each new term halves the remaining gap — visible convergence.

The ratio and root tests

For series with factorials or exponentials, compare a term to the one before it. Let L=lim⁡n→∞∣an+1an∣ \displaystyle L=\lim_{n\to\infty}\left|\frac{a_{n+1}}{a_n}\right| . Then the series converges absolutely if L<1 L\lt 1 , diverges if L>1 L\gt 1 , and the test is inconclusive if L=1 L=1 .

▲ Theorem 11.3 — Power series & radius of convergence

A power series ∑n=0∞cn(x−a)n \displaystyle\sum_{n=0}^{\infty}c_n(x-a)^{n} converges for all x x with ∣x−a∣<R |x-a|\lt R and diverges for ∣x−a∣>R |x-a|\gt R , where R R is the radius of convergence. The endpoints x=a±R x=a\pm R must be tested separately.

Geometric
converges iff ∣r∣<1 |r|\lt 1
p-series
converges iff p>1 p\gt 1
Ratio
L<1⇒ L\lt 1\Rightarrow converge
Alternating
terms ↓0⇒ \downarrow 0 \Rightarrow converge
Worked example 11.A — Ratio test

Test ∑n=1∞n2n \displaystyle\sum_{n=1}^{\infty}\frac{n}{2^{n}} for convergence.

Form the ratio of successive terms and take the limit:

L=lim⁡n→∞n+12n+1⋅2nn=lim⁡n→∞n+12n=12<1, L=\lim_{n\to\infty}\frac{n+1}{2^{n+1}}\cdot\frac{2^{n}}{n}=\lim_{n\to\infty}\frac{n+1}{2n}=\frac12\lt 1,

so the series converges absolutely.

Worked example 11.B — Radius of convergence

Find the radius of convergence of ∑n=0∞xnn! \displaystyle\sum_{n=0}^{\infty}\frac{x^{n}}{n!} .

The ratio of terms is ∣xn+1/(n+1)!xn/n!∣=∣x∣n+1→0 \left|\dfrac{x^{n+1}/(n+1)!}{x^{n}/n!}\right|=\dfrac{|x|}{n+1}\to 0 for every x x . Since L=0<1 L=0\lt 1 always, R=∞ R=\infty — this series (which is ex e^{x} ) converges everywhere.

Bar chart: Terms of Series an = n / 2^n with categories: n=1 (50), n=2 (50), n=3 (38), n=4 (25), n=5 (16), n=6 (9)013253850n=150n=250n=338n=425n=516n=69Terms of Series an = n / 2^n
Bar chart comparing term values an=n2na_n = \frac{n}{2^n} for n=1,…,6n = 1, \dots, 6, displaying rapid geometric decay toward 0 that drives convergence.
⚠ Common Traps & Exam Pitfalls
Ratio Test Inconclusiveness (L = 1): If L=lim⁡n→∞∣an+1an∣=1L = \lim_{n\to\infty} \left|\frac{a_{n+1}}{a_n}\right| = 1, the Ratio Test gives NO conclusion whatsoever. In particular, the Ratio Test ALWAYS gives L=1L = 1 for any p-series or rational fraction in nn; use the Comparison Test or Integral Test instead!

Testing Endpoints for Interval of Convergence: Finding the radius of convergence RR determines an open interval (a−R,a+R)(a - R, a + R). You MUST test each endpoint x=a−Rx = a - R and x=a+Rx = a + R separately, as convergence at boundaries varies (e.g. one end might be conditionally convergent via Alternating Series while the other diverges).

Absolute vs Conditional Convergence: A series ∑an\sum a_n is conditionally convergent if ∑an\sum a_n converges, but ∑∣an∣\sum |a_n| diverges (classic example: ∑(−1)n+1n\sum \frac{(-1)^{n+1}}{n}).
Find the radius of convergence RR of the power series ∑n=1∞(x−3)nn⋅5n\displaystyle\sum_{n=1}^{\infty} \frac{(x - 3)^n}{n \cdot 5^n}.
Apply the Ratio Test with an=(x−3)nn⋅5na_n = \frac{(x - 3)^n}{n \cdot 5^n}:
L=lim⁡n→∞∣an+1an∣=lim⁡n→∞∣(x−3)n+1(n+1)5n+1⋅n⋅5n(x−3)n∣=lim⁡n→∞nn+1⋅∣x−3∣5=∣x−3∣5. L = \lim_{n\to\infty} \left|\frac{a_{n+1}}{a_n}\right| = \lim_{n\to\infty} \left|\frac{(x - 3)^{n+1}}{(n+1)5^{n+1}} \cdot \frac{n \cdot 5^n}{(x - 3)^n}\right| = \lim_{n\to\infty} \frac{n}{n+1} \cdot \frac{|x - 3|}{5} = \frac{|x - 3|}{5}.
For absolute convergence, require L<1  ⟹  ∣x−3∣5<1  ⟹  ∣x−3∣<5L < 1 \implies \frac{|x - 3|}{5} < 1 \implies |x - 3| < 5. Thus the radius of convergence is R=5R = 5.
📝 Chapter Quiz
12

Vectors & Vector-Valued Functions

Multivariable calculus begins with vectors — quantities carrying both magnitude and direction. Letting a vector depend on a parameter traces a curve through space, and differentiating it recovers velocity and acceleration.

● Definition 12.1 — Vector and magnitude

A vector v=⟨v1,v2,v3⟩ \mathbf{v}=\langle v_1,v_2,v_3\rangle is an ordered triple with length ∣v∣=v12+v22+v32 \displaystyle|\mathbf{v}|=\sqrt{v_1^{2}+v_2^{2}+v_3^{2}} . Vectors add componentwise, and a unit vector is v^=v/∣v∣ \hat{\mathbf{v}}=\mathbf{v}/|\mathbf{v}| .

▲ Theorem 12.2 — Dot and cross products

The dot product u⋅v=∣u∣ ∣v∣cos⁡θ \mathbf{u}\cdot\mathbf{v}=|\mathbf{u}|\,|\mathbf{v}|\cos\theta measures alignment (zero when perpendicular). The cross product u×v \mathbf{u}\times\mathbf{v} has length ∣u∣ ∣v∣sin⁡θ |\mathbf{u}|\,|\mathbf{v}|\sin\theta and points perpendicular to both.

⊙ Explorer · Vector additioninteractive
v components⟨1.67, 1.99⟩
|u + v|5.10
resultant angle35.5°

Blue is u=⟨3,1⟩\mathbf u=\langle3,1\rangle, amber is v\mathbf v, dark is the resultant u+v\mathbf u+\mathbf v — the parallelogram diagonal.

r(t)⟨1.000, 0.000, 0.000⟩
|r′(t)| (speed)1.414

Vector-valued functions

A path in space is r(t)=⟨x(t),y(t),z(t)⟩ \mathbf{r}(t)=\langle x(t),y(t),z(t)\rangle . Differentiating component-by-component gives the velocity r′(t) \mathbf{r}'(t) , whose length ∣r′(t)∣ |\mathbf{r}'(t)| is the speed; differentiating again gives acceleration.

Dot product
u⋅v=u1v1+u2v2+u3v3 \mathbf{u}\cdot\mathbf{v}=u_1v_1+u_2v_2+u_3v_3
Unit vector
v^=v/∣v∣ \hat{\mathbf{v}}=\mathbf{v}/|\mathbf{v}|
Angle
cos⁡θ=u⋅v∣u∣ ∣v∣ \cos\theta=\dfrac{\mathbf{u}\cdot\mathbf{v}}{|\mathbf{u}|\,|\mathbf{v}|}
Velocity
r′(t)=⟨x′,y′,z′⟩ \mathbf{r}'(t)=\langle x',y',z'\rangle
Worked example 12.A — Angle between vectors

Find the angle between u=⟨1,2,2⟩ \mathbf{u}=\langle 1,2,2\rangle and v=⟨2,0,1⟩ \mathbf{v}=\langle 2,0,1\rangle .

Here u⋅v=2+0+2=4 \mathbf{u}\cdot\mathbf{v}=2+0+2=4 , ∣u∣=3 |\mathbf{u}|=3 , ∣v∣=5 |\mathbf{v}|=\sqrt5 , so

cos⁡θ=435≈0.596⇒θ≈53.4∘. \cos\theta=\frac{4}{3\sqrt5}\approx 0.596 \quad\Rightarrow\quad \theta\approx 53.4^{\circ}.

Worked example 12.B — Velocity and speed

For the helix r(t)=⟨cos⁡t,sin⁡t,t⟩ \mathbf{r}(t)=\langle\cos t,\sin t,t\rangle , find the velocity and speed.

Differentiating each component, r′(t)=⟨−sin⁡t,cos⁡t,1⟩ \mathbf{r}'(t)=\langle-\sin t,\cos t,1\rangle . Its length is constant:

∣r′(t)∣=sin⁡2t+cos⁡2t+1=2. |\mathbf{r}'(t)|=\sqrt{\sin^{2}t+\cos^{2}t+1}=\sqrt2.

Triangle Originvx(vx, vy) with sides vx = 4, vy = 3, |v| = 5 and angles θ, 90°; right angle at vxOriginvx(vx, vy)vx = 4vy = 3|v| = 5θ90°
Right-angled vector component decomposition in 2D space, demonstrating ∣v⃗∣=vx2+vy2|\vec v| = \sqrt{v_x^2 + v_y^2} and orthogonal directions.
⚠ Common Traps & Exam Pitfalls
Dot Product vs Cross Product Output: The dot product u⃗⋅v⃗=u1v1+u2v2+u3v3\vec u \cdot \vec v = u_1v_1 + u_2v_2 + u_3v_3 produces a SCALAR (number). The cross product u⃗×v⃗\vec u \times \vec v produces a VECTOR perpendicular to both original vectors.

Cross Product Anti-Commutativity: Order of factors reverses the sign: u⃗×v⃗=−(v⃗×u⃗)\vec u \times \vec v = -(\vec v \times \vec u). Swapping vector order flips the resulting direction (Right-Hand Rule).

Unit Tangent Vector Normalization: The unit tangent vector T⃗(t)=r⃗′(t)∣r⃗′(t)∣\vec T(t) = \frac{\vec r'(t)}{|\vec r'(t)|} requires dividing velocity by speed. Forgetting to divide by magnitude leaves a velocity vector with non-unit length.
Determine whether the vectors u⃗=⟨2,−3,4⟩\vec u = \langle 2, -3, 4\rangle and v⃗=⟨6,8,3⟩\vec v = \langle 6, 8, 3\rangle are orthogonal, parallel, or neither.
Compute the dot product:
u⃗⋅v⃗=(2)(6)+(−3)(8)+(4)(3)=12−24+12=0. \vec u \cdot \vec v = (2)(6) + (-3)(8) + (4)(3) = 12 - 24 + 12 = 0.
Since the dot product is zero and neither vector is the zero vector, u⃗\vec u and v⃗\vec v are strictly orthogonal (perpendicular).
📝 Chapter Quiz
13

Partial Derivatives & the Gradient

For a surface z=f(x,y) z=f(x,y) , there is no single slope — it depends on the direction you walk. Partial derivatives measure the slope along each axis, and the gradient bundles them into the direction of steepest ascent.

● Definition 13.1 — Partial derivative

The partial derivative fx=∂f∂x \displaystyle f_x=\frac{\partial f}{\partial x} differentiates f f with respect to x x while holding y y constant; fy f_y does the reverse. Geometrically, fx f_x is the slope of the curve where the surface is sliced by a plane of fixed y y .

▲ Theorem 13.2 — Gradient & directional derivative

The gradient ∇f=⟨fx,fy⟩ \nabla f=\langle f_x,f_y\rangle points in the direction of greatest increase, with rate ∣∇f∣ |\nabla f| . The slope in a unit direction u \mathbf{u} is the directional derivative Duf=∇f⋅u D_{\mathbf{u}}f=\nabla f\cdot\mathbf{u} .

⊙ Explorer · Slicing a surfaceinteractive
f(1, c)2.800
fx(1, c)-0.400

Fixing y=cy=c gives the curve g(x)=f(x,c)g(x)=f(x,c). Its slope at x=1x=1 is the partial fx(1,c)f_x(1,c) — and it shifts as cc moves.

Tangent planes and local extrema

Near a point, a smooth surface looks flat. The tangent plane at (a,b) (a,b) is

z=f(a,b)+fx(a,b)(x−a)+fy(a,b)(y−b). z=f(a,b)+f_x(a,b)(x-a)+f_y(a,b)(y-b).

Local maxima and minima occur where ∇f=0 \nabla f=\mathbf{0} ; the second-derivative test uses D=fxxfyy−fxy2 D=f_{xx}f_{yy}-f_{xy}^{2} to classify them (D>0 D\gt 0 and fxx>0 f_{xx}\gt 0 gives a minimum).

Partial
∂f∂x \dfrac{\partial f}{\partial x}
Gradient
∇f=⟨fx,fy⟩ \nabla f=\langle f_x,f_y\rangle
Directional
Duf=∇f⋅u D_{\mathbf{u}}f=\nabla f\cdot\mathbf{u}
Second test
D=fxxfyy−fxy2 D=f_{xx}f_{yy}-f_{xy}^{2}
Worked example 13.A — Computing partials

For f(x,y)=x2y+sin⁡(xy) f(x,y)=x^{2}y+\sin(xy) , find fx f_x and fy f_y .

Treating y y as constant for fx f_x , then x x as constant for fy f_y :

fx=2xy+ycos⁡(xy),fy=x2+xcos⁡(xy). f_x=2xy+y\cos(xy), \qquad f_y=x^{2}+x\cos(xy).

Worked example 13.B — Gradient and steepest ascent

For f(x,y)=x2+y2 f(x,y)=x^{2}+y^{2} , find the gradient at (1,2) (1,2) and the direction of fastest increase.

Since ∇f=⟨2x,2y⟩ \nabla f=\langle 2x,2y\rangle , at (1,2) (1,2) we get ∇f=⟨2,4⟩ \nabla f=\langle 2,4\rangle . Fastest increase is along this vector, i.e. the unit direction

u^=120⟨2,4⟩,rate ∣∇f∣=20=25. \hat{\mathbf{u}}=\frac{1}{\sqrt{20}}\langle 2,4\rangle, \qquad \text{rate } |\nabla f|=\sqrt{20}=2\sqrt5.

Circle centered at O(0,0) with radius √5 with shaded sector ∇f direction∇f directionO(0,0)√5
Level curves of paraboloid z=x2+y2z = x^2 + y^2 showing concentric circular contours and gradient vector ∇f=⟨2,4⟩\nabla f = \langle 2, 4\rangle orthogonal to the contour at (1,2)(1, 2).
⚠ Common Traps & Exam Pitfalls
Directional Derivative Requires a Unit Vector: The formula is Du⃗f=∇f⋅u^D_{\vec u}f = \nabla f \cdot \hat u. If the problem gives an arbitrary direction v⃗\vec v, you MUST divide by its magnitude ∣v⃗∣|\vec v| first. Forgetting to normalize scales the directional derivative by ∣v⃗∣|\vec v| and produces an incorrect rate.

Gradient Geometric Meaning: ∇f(a,b)\nabla f(a, b) points in the direction of maximum rate of increase, and its magnitude ∣∇f∣|\nabla f| is that maximum rate. Crucially, the gradient vector is ALWAYS orthogonal (perpendicular) to the level curve f(x,y)=cf(x, y) = c at that point.

Second Derivative Test Discriminant: D=fxxfyy−(fxy)2D = f_{xx}f_{yy} - (f_{xy})^2. If D<0D < 0, the point is a saddle point regardless of the sign of fxxf_{xx}.
Find the directional derivative of f(x,y)=3x2y−y3f(x, y) = 3x^2y - y^3 at the point (1,2)(1, 2) in the direction of v⃗=⟨3,4⟩\vec v = \langle 3, 4\rangle.
First compute the gradient: ∇f=⟨6xy,3x2−3y2⟩\nabla f = \langle 6xy, 3x^2 - 3y^2\rangle.
At (1,2)(1, 2): ∇f(1,2)=⟨6(1)(2),3(1)2−3(2)2⟩=⟨12,3−12⟩=⟨12,−9⟩\nabla f(1, 2) = \langle 6(1)(2), 3(1)^2 - 3(2)^2\rangle = \langle 12, 3 - 12\rangle = \langle 12, -9\rangle.
Normalize the direction vector v⃗\vec v: ∣v⃗∣=32+42=5|\vec v| = \sqrt{3^2 + 4^2} = 5, so u^=⟨35,45⟩\hat u = \langle \frac{3}{5}, \frac{4}{5}\rangle.
Compute the dot product:
Du⃗f(1,2)=∇f⋅u^=12(35)+(−9)(45)=36−365=0. D_{\vec u}f(1, 2) = \nabla f \cdot \hat u = 12\left(\frac{3}{5}\right) + (-9)\left(\frac{4}{5}\right) = \frac{36 - 36}{5} = 0.
📝 Chapter Quiz
14

Multiple Integrals

A single integral accumulates over an interval; a double integral accumulates a function over a two-dimensional region — most concretely, the volume trapped under a surface z=f(x,y) z=f(x,y) .

● Definition 14.1 — The double integral

Partition a region R R into small cells of area ΔA \Delta A , sample f f in each, and sum. The double integral is the limit as the cells shrink:

∬Rf dA=lim⁡ΔA→0∑i,jf(xi,yj) ΔA. \iint_{R} f\,dA=\lim_{\Delta A\to 0}\sum_{i,j} f(x_i,y_j)\,\Delta A.

▲ Theorem 14.2 — Fubini's theorem

Over a rectangle R=[a,b]×[c,d] R=[a,b]\times[c,d] , a double integral equals an iterated integral, and the order may be swapped:

∬Rf dA=∫ab ⁣ ⁣∫cdf(x,y) dy dx=∫cd ⁣ ⁣∫abf(x,y) dx dy. \iint_{R} f\,dA=\int_a^b\!\!\int_c^d f(x,y)\,dy\,dx=\int_c^d\!\!\int_a^b f(x,y)\,dx\,dy.

⊙ Explorer · Double Riemann suminteractive
cells16
approx ∬ f dA8.000
exact value8

Each cell is shaded by f=x+yf=x+y at its midpoint over [0,2]2[0,2]^2. Refine the grid and the midpoint sum converges to 88.

Double integrals in polar coordinates

For circular regions, polar coordinates simplify everything — but the area element gains a factor of r r :

∬Rf dA=∬f(rcos⁡θ, rsin⁡θ) r dr dθ. \iint_{R} f\,dA=\iint f(r\cos\theta,\,r\sin\theta)\,r\,dr\,d\theta.

That extra r r is the Jacobian of the polar change of variables, and forgetting it is the most common error in the topic.

Double integral
∬Rf dA \iint_R f\,dA
Iterated
∫ ⁣ ⁣∫f dy dx \int\!\!\int f\,dy\,dx
Area
∬RdA \iint_R dA
Polar
r dr dθ r\,dr\,d\theta
Worked example 14.A — An iterated integral

Evaluate ∫01 ⁣ ⁣∫02(x+2y) dx dy \displaystyle\int_0^1\!\!\int_0^2 (x+2y)\,dx\,dy .

Integrate in x x first, treating y y as constant:

∫01[x22+2xy]02dy=∫01(2+4y) dy=[2y+2y2]01=4. \int_0^1\Big[\tfrac{x^{2}}{2}+2xy\Big]_0^2 dy=\int_0^1(2+4y)\,dy=\big[2y+2y^{2}\big]_0^1=4.

Worked example 14.B — Area of a disk in polar

Confirm the area of the unit disk x2+y2≤1 x^{2}+y^{2}\le 1 using a polar double integral.

∬RdA=∫02π ⁣ ⁣∫01r dr dθ=∫02π12 dθ=π. \iint_{R} dA=\int_0^{2\pi}\!\!\int_0^1 r\,dr\,d\theta=\int_0^{2\pi}\tfrac12\,d\theta=\pi.

Rectangle (0,0)(2,0)(2,1)(0,1) with sides Δx = 2, Δy = 1, Δx = 2, Δy = 1(0,0)(2,0)(2,1)(0,1)Δx = 2Δy = 1Δx = 2Δy = 1
Rectangular region of integration R=[0,2]×[0,1]R = [0, 2] \times [0, 1] in the xyxy-plane for double integral evaluation.
⚠ Common Traps & Exam Pitfalls
Polar Area Element (Jacobian r): In polar coordinates, dA=r dr dθdA = r\,dr\,d\theta. Omitting the extra factor of rr is the single most common error in multivariable calculus!

Reversing Order of Integration: You CANNOT merely swap the integral signs and limits when the region is non-rectangular: ∫01∫x1f(x,y) dy dx≠∫x1∫01f(x,y) dx dy\int_0^1 \int_x^1 f(x,y)\,dy\,dx \ne \int_x^1 \int_0^1 f(x,y)\,dx\,dy. You MUST sketch the 2D domain and reconstruct the bounding functions from horizontal vs vertical slices.

Coordinate Transformations Jacobian: When substituting x=g(u,v)x = g(u, v), y=h(u,v)y = h(u, v), always multiply the integrand by the absolute value of the Jacobian determinant ∣J(u,v)∣=∣xuyv−xvyu∣|J(u, v)| = |x_u y_v - x_v y_u|.
Evaluate ∬R(2x+y) dA\displaystyle\iint_R (2x + y)\,dA where RR is the rectangular region [0,3]×[1,2][0, 3] \times [1, 2].
Set up iterated integral:
∫12∫03(2x+y) dx dy=∫12[x2+xy]03dy=∫12(9+3y) dy \int_1^2 \int_0^3 (2x + y)\,dx\,dy = \int_1^2 \left[ x^2 + xy \right]_0^3 dy = \int_1^2 (9 + 3y)\,dy
Integrate with respect to yy:
[9y+3y22]12=(18+122)−(9+32)=24−10.5=13.5=272. \left[ 9y + \frac{3y^2}{2} \right]_1^2 = \left(18 + \frac{12}{2}\right) - \left(9 + \frac{3}{2}\right) = 24 - 10.5 = 13.5 = \frac{27}{2}.
📝 Chapter Quiz
15

Vector Calculus

The capstone of Calc III integrates vector fields — assignments of a vector to every point — along curves and across surfaces. Three great theorems (Green, Stokes, Divergence) tie these integrals back to the derivatives ∇⋅F \nabla\cdot\mathbf{F} and ∇×F \nabla\times\mathbf{F} .

● Definition 15.1 — Line integral & work

The line integral ∫CF⋅dr \displaystyle\int_C \mathbf{F}\cdot d\mathbf{r} measures the work a field F \mathbf{F} does along a curve C C . A field is conservative when F=∇f \mathbf{F}=\nabla f for some f f ; then the integral is path-independent and equals f(end)−f(start) f(\text{end})-f(\text{start}) .

▲ Theorem 15.2 — Green's theorem

For a positively oriented simple closed curve C C bounding a region R R in the plane,

∮C(P dx+Q dy)=∬R(∂Q∂x−∂P∂y) dA. \oint_C \big(P\,dx+Q\,dy\big)=\iint_{R}\Big(\frac{\partial Q}{\partial x}-\frac{\partial P}{\partial y}\Big)\,dA.

⊙ Explorer · Vector field — divergence & curlinteractive
divergence ∇·F0.00
curl ∇×F2.00
field typerotational

At t=1t=1 the field is ⟨−y,x⟩\langle -y,x\rangle (pure rotation, curl 22); at t=0t=0 it is ⟨x,y⟩\langle x,y\rangle (pure source, divergence 22).

Stokes' and the Divergence theorems

Green's theorem generalizes in two directions. Stokes' theorem relates circulation around a boundary curve to the curl over a surface; the Divergence theorem relates outward flux through a closed surface to the divergence inside:

∮CF⋅dr=∬S(∇×F)⋅dS,∬SF⋅dS=∭E(∇⋅F) dV. \oint_C \mathbf{F}\cdot d\mathbf{r}=\iint_S (\nabla\times\mathbf{F})\cdot d\mathbf{S}, \qquad \iint_S \mathbf{F}\cdot d\mathbf{S}=\iiint_E (\nabla\cdot\mathbf{F})\,dV.

Line integral
∫CF⋅dr \int_C \mathbf{F}\cdot d\mathbf{r}
Green
∮=∬( Qx−Py) \oint=\iint(\,Q_x-P_y)
Divergence
∇⋅F \nabla\cdot\mathbf{F}
Curl
∇×F \nabla\times\mathbf{F}
Worked example 15.A — Green's theorem

Evaluate ∮C(−y dx+x dy) \displaystyle\oint_C (-y\,dx+x\,dy) around the unit circle, counterclockwise.

Here P=−y, Q=x P=-y,\ Q=x , so Qx−Py=1−(−1)=2 Q_x-P_y=1-(-1)=2 . By Green's theorem,

∮C(−y dx+x dy)=∬R2 dA=2(area of disk)=2π. \oint_C(-y\,dx+x\,dy)=\iint_{R}2\,dA=2(\text{area of disk})=2\pi.

Worked example 15.B — The Divergence theorem

Find the outward flux of F=⟨x,y,z⟩ \mathbf{F}=\langle x,y,z\rangle through the unit sphere.

Since ∇⋅F=1+1+1=3 \nabla\cdot\mathbf{F}=1+1+1=3 , the Divergence theorem turns the surface flux into a volume integral over the unit ball E E :

∬SF⋅dS=∭E3 dV=3⋅43π=4π. \iint_S \mathbf{F}\cdot d\mathbf{S}=\iiint_E 3\,dV=3\cdot\tfrac{4}{3}\pi=4\pi.

Circle centered at O(0,0) with radius 1 with shaded sector C (counterclockwise)C (counterclockwise)O(0,0)1
Positively oriented (counterclockwise) closed boundary curve CC enclosing planar region RR for Green's Theorem.
⚠ Common Traps & Exam Pitfalls
Green's Theorem Orientation: Green's Theorem ∮C(P dx+Q dy)=∬R(Qx−Py) dA\oint_C (P\,dx + Q\,dy) = \iint_R (Q_x - P_y)\,dA strictly requires a positively oriented (counterclockwise) boundary curve CC keeping the region on the left. If traversing clockwise, you MUST insert a negative sign!

Conservative Vector Fields Checklist: A vector field F⃗=∇f\vec F = \nabla f has curl(F⃗)=0⃗\text{curl}(\vec F) = \vec 0. On simply connected domains: (1) Path independence ∫C1=∫C2\int_{C_1} = \int_{C_2}; (2) Zero work around any closed loop: ∮CF⃗⋅dr⃗=0\oint_C \vec F \cdot d\vec r = 0; (3) Fundamental Theorem for Line Integrals: ∫C∇f⋅dr⃗=f(B)−f(A)\int_C \nabla f \cdot d\vec r = f(B) - f(A).

Divergence vs Curl: Divergence ∇⋅F⃗\nabla \cdot \vec F yields a scalar measuring net outflow; Curl ∇×F⃗\nabla \times \vec F yields a vector measuring rotational circulation.
Use Green's Theorem to evaluate ∮C(3y dx+5x dy)\displaystyle\oint_C (3y\,dx + 5x\,dy) where CC is the counterclockwise circle x2+y2=4x^2 + y^2 = 4.
Identify components: P=3yP = 3y and Q=5xQ = 5x.
Compute partial derivatives: ∂Q∂x=5\frac{\partial Q}{\partial x} = 5 and ∂P∂y=3\frac{\partial P}{\partial y} = 3.
Apply Green's Theorem:
∮C(3y dx+5x dy)=∬R(∂Q∂x−∂P∂y) dA=∬R(5−3) dA=2∬RdA. \oint_C (3y\,dx + 5x\,dy) = \iint_R \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right)\,dA = \iint_R (5 - 3)\,dA = 2 \iint_R dA.
The region RR is a disk of radius r=2r = 2, so its area is π(22)=4π\pi(2^2) = 4\pi.
Therefore, 2∬RdA=2(4π)=8π2 \iint_R dA = 2(4\pi) = 8\pi.
📝 Chapter Quiz
§

Practice set

Fifty mixed problems spanning all ten chapters, ordered roughly from limits to series and tagged by difficulty. Click any problem to reveal a complete worked solution.

P1

Evaluate lim⁡x→2x2−4x−2 \displaystyle\lim_{x\to 2}\frac{x^2-4}{x-2} .

Basic

Factor: x2−4=(x−2)(x+2) x^2-4=(x-2)(x+2) . Cancel (x−2) (x-2) :

lim⁡x→2(x+2)=4. \lim_{x\to 2}(x+2)=4.
P2

Differentiate f(x)=5x4−3x2+7 f(x)=5x^4-3x^2+7 .

Basic

Apply the power and sum rules term by term:

f′(x)=20x3−6x. f'(x)=20x^3-6x.
P3

Differentiate y=xx2+1 y=\dfrac{x}{x^2+1} .

Intermediate

Quotient rule with f=x, g=x2+1 f=x,\ g=x^2+1 , so f′=1, g′=2x f'=1,\ g'=2x :

y′=(1)(x2+1)−(x)(2x)(x2+1)2=1−x2(x2+1)2. y'=\frac{(1)(x^2+1)-(x)(2x)}{(x^2+1)^2}=\frac{1-x^2}{(x^2+1)^2}.
P4

Differentiate y=e2xcos⁡x y=e^{2x}\cos x .

Intermediate

Product rule; the first factor needs the chain rule, ddxe2x=2e2x \tfrac{d}{dx}e^{2x}=2e^{2x} :

y′=2e2xcos⁡x−e2xsin⁡x=e2x(2cos⁡x−sin⁡x). y'=2e^{2x}\cos x - e^{2x}\sin x = e^{2x}\big(2\cos x-\sin x\big).
P5

Evaluate ∫13(2x+1) dx \displaystyle\int_1^{3}\big(2x+1\big)\,dx .

Basic

Antiderivative x2+x x^2+x . By the Fundamental Theorem:

[x2+x]13=(9+3)−(1+1)=12−2=10. \big[x^2+x\big]_1^{3}=(9+3)-(1+1)=12-2=10.
P6

Find the area under f(x)=sin⁡x f(x)=\sin x over [0,π2] \big[0,\tfrac{\pi}{2}\big] .

Intermediate

Use ∫sin⁡x dx=−cos⁡x \int \sin x\,dx=-\cos x :

∫0π/2sin⁡x dx=[−cos⁡x]0π/2=0−(−1)=1. \int_0^{\pi/2}\sin x\,dx=\big[-\cos x\big]_0^{\pi/2}=0-(-1)=1.
P7

Differentiate y=(3x2+1)5 y=\big(3x^2+1\big)^{5} .

Advanced

Chain rule: outer power u5 u^5 gives 5u4 5u^4 ; inner derivative ddx(3x2+1)=6x \tfrac{d}{dx}(3x^2+1)=6x :

y′=5(3x2+1)4⋅6x=30x(3x2+1)4. y'=5\big(3x^2+1\big)^{4}\cdot 6x=30x\big(3x^2+1\big)^{4}.
P8

A particle's position is s(t)=t3−6t2+9t s(t)=t^3-6t^2+9t . Find the times when it is momentarily at rest.

Advanced

Velocity is the derivative; rest means v(t)=0 v(t)=0 :

v(t)=s′(t)=3t2−12t+9=3(t−1)(t−3). v(t)=s'(t)=3t^2-12t+9=3(t-1)(t-3).

So the particle is at rest at t=1 t=1 and t=3 t=3 .

P9

Find and classify the local extrema of f(x)=2x3−9x2+12x f(x)=2x^3-9x^2+12x .

Advanced

f′(x)=6x2−18x+12=6(x−1)(x−2) f'(x)=6x^2-18x+12=6(x-1)(x-2) , so critical points at x=1,2 x=1,2 . With f′′(x)=12x−18 f''(x)=12x-18 :

f′′(1)=−6<0 (max),f′′(2)=6>0 (min). f''(1)=-6<0\ (\text{max}),\quad f''(2)=6>0\ (\text{min}).

Local maximum (1,5) (1,5) , local minimum (2,4) (2,4) .

P10

Evaluate ∫xsin⁡ ⁣(x2) dx \displaystyle\int x\sin\!\big(x^2\big)\,dx .

Intermediate

Let u=x2 u=x^2 , so du=2x dx du=2x\,dx and x dx=12 du x\,dx=\tfrac12\,du :

∫xsin⁡ ⁣(x2) dx=12∫sin⁡u du=−12cos⁡ ⁣(x2)+C. \int x\sin\!\big(x^2\big)\,dx=\tfrac12\int\sin u\,du=-\tfrac12\cos\!\big(x^2\big)+C.
P11

Find the area enclosed between y=4−x2 y=4-x^2 and y=x+2 y=x+2 .

Advanced

Intersections: 4−x2=x+2⇒x2+x−2=0⇒x=−2,1 4-x^2=x+2\Rightarrow x^2+x-2=0\Rightarrow x=-2,1 . The parabola is on top, so

∫−21[(4−x2)−(x+2)] dx=∫−21(2−x−x2) dx=92. \int_{-2}^{1}\big[(4-x^2)-(x+2)\big]\,dx=\int_{-2}^{1}\big(2-x-x^2\big)\,dx=\frac{9}{2}.
P12

Evaluate ∑n=1∞3(14)n \displaystyle\sum_{n=1}^{\infty} 3\Big(\tfrac{1}{4}\Big)^{n} .

Intermediate

The first term (at n=1 n=1 ) is a=34 a=\tfrac34 and the ratio is r=14 r=\tfrac14 :

∑n=1∞3(14)n=a1−r=3/43/4=1. \sum_{n=1}^{\infty} 3\Big(\tfrac14\Big)^{n}=\frac{a}{1-r}=\frac{3/4}{3/4}=1.
P13

Solve the separable equation dydx=xy \dfrac{dy}{dx}=\dfrac{x}{y} .

Intermediate

Separate: y dy=x dx y\,dy=x\,dx . Integrate both sides:

y22=x22+C ⟹ y2−x2=C. \tfrac{y^2}{2}=\tfrac{x^2}{2}+C\ \Longrightarrow\ y^2-x^2=C.
P14

For x=t2, y=t3 x=t^2,\ y=t^3 , find dydx \dfrac{dy}{dx} .

Intermediate
dydx=dy/dtdx/dt=3t22t=3t2. \frac{dy}{dx}=\frac{dy/dt}{dx/dt}=\frac{3t^2}{2t}=\frac{3t}{2}.
P15

Evaluate lim⁡x→01−cos⁡xx2 \displaystyle\lim_{x\to 0}\frac{1-\cos x}{x^2} .

Advanced

Form 00 \tfrac00 ; apply L'Hôpital twice:

lim⁡x→01−cos⁡xx2=lim⁡x→0sin⁡x2x=lim⁡x→0cos⁡x2=12. \lim_{x\to 0}\frac{1-\cos x}{x^2}=\lim_{x\to 0}\frac{\sin x}{2x}=\lim_{x\to 0}\frac{\cos x}{2}=\frac12.
P16

Evaluate lim⁡x→2(3x2−x+1) \displaystyle\lim_{x\to 2}\big(3x^2-x+1\big) .

Basic

The polynomial is continuous, so substitute directly:

3(2)2−2+1=11. 3(2)^2-2+1=11.
P17

Evaluate lim⁡x→0sin⁡3xx \displaystyle\lim_{x\to 0}\frac{\sin 3x}{x} .

Basic

Use lim⁡u→0sin⁡uu=1 \lim_{u\to 0}\tfrac{\sin u}{u}=1 :

lim⁡x→0sin⁡3xx=3lim⁡x→0sin⁡3x3x=3. \lim_{x\to 0}\frac{\sin 3x}{x}=3\lim_{x\to 0}\frac{\sin 3x}{3x}=3.
P18

Evaluate lim⁡x→∞2x2−3x+15x2+x \displaystyle\lim_{x\to\infty}\frac{2x^2-3x+1}{5x^2+x} .

Intermediate

Divide by x2 x^2 ; lower-order terms vanish, leaving the ratio of leading coefficients:

25. \frac{2}{5}.
P19

Evaluate lim⁡x→0x+4−2x \displaystyle\lim_{x\to 0}\frac{\sqrt{x+4}-2}{x} .

Intermediate

Multiply by the conjugate x+4+2 \sqrt{x+4}+2 :

lim⁡x→0(x+4)−4x(x+4+2)=lim⁡x→01x+4+2=14. \lim_{x\to 0}\frac{(x+4)-4}{x\big(\sqrt{x+4}+2\big)}=\lim_{x\to 0}\frac{1}{\sqrt{x+4}+2}=\frac14.
P20

Find k k so that f(x)={x2,x≤1kx,x>1 f(x)=\begin{cases} x^2,&x\le 1\\ kx,&x>1\end{cases} is continuous at x=1 x=1 .

Intermediate

The two pieces must agree at x=1 x=1 : 12=k(1) 1^2=k(1) .

k=1. k=1.
P21

Differentiate f(x)=7x3−4x+9 f(x)=7x^3-4x+9 .

Basic
f′(x)=21x2−4. f'(x)=21x^2-4.
P22

Differentiate y=cos⁡5x y=\cos 5x .

Basic

Chain rule with inner 5x 5x :

y′=−5sin⁡5x. y'=-5\sin 5x.
P23

Differentiate y=e2x y=e^{2x} .

Basic
y′=2e2x. y'=2e^{2x}.
P24

Differentiate y=ln⁡(3x) y=\ln(3x) .

Basic

Chain rule: 13x⋅3 \tfrac{1}{3x}\cdot 3 .

y′=1x. y'=\frac1x.
P25

Differentiate y=x3ln⁡x y=x^3\ln x .

Intermediate

Product rule: 3x2ln⁡x+x3⋅1x 3x^2\ln x + x^3\cdot\tfrac1x .

y′=x2(3ln⁡x+1). y'=x^2\big(3\ln x+1\big).
P26

Differentiate y=xx+1 y=\dfrac{x}{x+1} .

Intermediate

Quotient rule:

y′=(1)(x+1)−x(1)(x+1)2=1(x+1)2. y'=\frac{(1)(x+1)-x(1)}{(x+1)^2}=\frac{1}{(x+1)^2}.
P27

Differentiate y=x2+1 y=\sqrt{x^2+1} .

Intermediate

Chain rule on (x2+1)1/2 (x^2+1)^{1/2} :

y′=xx2+1. y'=\frac{x}{\sqrt{x^2+1}}.
P28

Differentiate y=tan⁡3x y=\tan 3x .

Intermediate
y′=3sec⁡23x. y'=3\sec^2 3x.
P29

Find dydx \dfrac{dy}{dx} if x2+y2=25 x^2+y^2=25 .

Advanced

Differentiate implicitly: 2x+2y y′=0 2x+2y\,y'=0 .

dydx=−xy. \frac{dy}{dx}=-\frac{x}{y}.
P30

Find dydx \dfrac{dy}{dx} if xy+y2=6 xy+y^2=6 .

Advanced

Differentiate implicitly (product rule on xy xy ): y+x y′+2y y′=0 y+x\,y'+2y\,y'=0 .

dydx=−yx+2y. \frac{dy}{dx}=-\frac{y}{x+2y}.
P31

Find the tangent line to y=x2 y=x^2 at x=3 x=3 .

Intermediate

Point (3,9) (3,9) ; slope y′=2x=6 y'=2x=6 . Then y−9=6(x−3) y-9=6(x-3) :

y=6x−9. y=6x-9.
P32

On what intervals is f(x)=x3−3x f(x)=x^3-3x increasing?

Intermediate

f′(x)=3x2−3>0⇒x2>1 f'(x)=3x^2-3>0 \Rightarrow x^2>1 :

x<−1 or x>1. x<-1 \ \text{or}\ x>1.
P33

A rectangular field is enclosed with 60 m of fencing on all four sides. What dimensions maximise the area?

Advanced

With l+w=30 l+w=30 , area A=l(30−l) A=l(30-l) , so A′(l)=30−2l=0⇒l=15 A'(l)=30-2l=0\Rightarrow l=15 .

15×15,Amax⁡=225 m2. 15\times 15,\qquad A_{\max}=225\ \text{m}^2.
P34

A 10 m ladder leans on a wall; its base slides away at 1 m/s. How fast is the top sliding down when the base is 6 m from the wall?

Advanced

From x2+y2=100 x^2+y^2=100 , at x=6 x=6 we get y=8 y=8 . Differentiate: 2x x′+2y y′=0 2x\,x'+2y\,y'=0 :

y′=−x x′y=−6(1)8=−0.75 m/s. y'=-\frac{x\,x'}{y}=-\frac{6(1)}{8}=-0.75\ \text{m/s}.

The top slides down at 0.75 0.75 m/s.

P35

Evaluate lim⁡x→0ex−1x \displaystyle\lim_{x\to 0}\frac{e^{x}-1}{x} .

Intermediate

Form 00 \tfrac00 ; by L'Hôpital, lim⁡ex/1 \lim e^{x}/1 :

=1. =1.
P36

Evaluate ∫(6x2−4x+3) dx \displaystyle\int \big(6x^2-4x+3\big)\,dx .

Basic
2x3−2x2+3x+C. 2x^3-2x^2+3x+C.
P37

Evaluate ∫01ex dx \displaystyle\int_0^{1} e^{x}\,dx .

Basic
[ex]01=e−1. \big[e^{x}\big]_0^{1}=e-1.
P38

Evaluate ∫1e1x dx \displaystyle\int_1^{e}\frac{1}{x}\,dx .

Basic
[ln⁡x]1e=ln⁡e−ln⁡1=1. \big[\ln x\big]_1^{e}=\ln e-\ln 1=1.
P39

Evaluate ∫0π/2cos⁡x dx \displaystyle\int_0^{\pi/2}\cos x\,dx .

Intermediate
[sin⁡x]0π/2=1−0=1. \big[\sin x\big]_0^{\pi/2}=1-0=1.
P40

Evaluate ∫04x dx \displaystyle\int_0^{4}\sqrt{x}\,dx .

Intermediate

Write x=x1/2 \sqrt{x}=x^{1/2} :

[23x3/2]04=23(8)=163. \Big[\tfrac{2}{3}x^{3/2}\Big]_0^{4}=\tfrac{2}{3}(8)=\frac{16}{3}.
P41

Evaluate ∫2x ex2 dx \displaystyle\int 2x\,e^{x^2}\,dx .

Intermediate

Let u=x2 u=x^2 , du=2x dx du=2x\,dx :

∫eu du=ex2+C. \int e^{u}\,du=e^{x^2}+C.
P42

Evaluate ∫xcos⁡x dx \displaystyle\int x\cos x\,dx .

Intermediate

By parts with u=x, dv=cos⁡x dx u=x,\ dv=\cos x\,dx :

xsin⁡x−∫sin⁡x dx=xsin⁡x+cos⁡x+C. x\sin x-\int\sin x\,dx=x\sin x+\cos x+C.
P43

Evaluate ∫ln⁡x dx \displaystyle\int \ln x\,dx .

Advanced

By parts with u=ln⁡x, dv=dx u=\ln x,\ dv=dx :

xln⁡x−∫x⋅1x dx=xln⁡x−x+C. x\ln x-\int x\cdot\tfrac1x\,dx=x\ln x-x+C.
P44

Evaluate ∫2x+1x2+x dx \displaystyle\int \frac{2x+1}{x^2+x}\,dx .

Intermediate

The numerator is the derivative of the denominator, so let u=x2+x u=x^2+x :

∫duu=ln⁡∣x2+x∣+C. \int\frac{du}{u}=\ln\big|x^2+x\big|+C.
P45

Find the area under y=4−x2 y=4-x^2 from x=−2 x=-2 to x=2 x=2 .

Intermediate
∫−22(4−x2) dx=[4x−x33]−22=323. \int_{-2}^{2}\big(4-x^2\big)\,dx=\Big[4x-\tfrac{x^3}{3}\Big]_{-2}^{2}=\frac{32}{3}.
P46

The region under y=x y=x from 0 0 to 2 2 is revolved about the x x -axis. Find the volume.

Advanced

Disk method with R(x)=x R(x)=x :

π∫02x2 dx=π[x33]02=8π3. \pi\int_0^{2}x^2\,dx=\pi\Big[\tfrac{x^3}{3}\Big]_0^{2}=\frac{8\pi}{3}.
P47

Find the average value of f(x)=x2 f(x)=x^2 on [0,3] [0,3] .

Intermediate
fˉ=13∫03x2 dx=13⋅9=3. \bar f=\frac{1}{3}\int_0^{3}x^2\,dx=\frac{1}{3}\cdot 9=3.
P48

Solve dydx=2y \dfrac{dy}{dx}=2y with y(0)=5 y(0)=5 .

Intermediate

Exponential model y=y0ekt y=y_0e^{kt} with k=2 k=2 , y0=5 y_0=5 :

y=5e2x. y=5e^{2x}.
P49

For x=t2, y=2t x=t^2,\ y=2t , find dydx \dfrac{dy}{dx} .

Intermediate
dydx=dy/dtdx/dt=22t=1t. \frac{dy}{dx}=\frac{dy/dt}{dx/dt}=\frac{2}{2t}=\frac{1}{t}.
P50

Evaluate ∑n=0∞(23)n \displaystyle\sum_{n=0}^{\infty}\Big(\tfrac{2}{3}\Big)^{n} .

Intermediate

Geometric with a=1, r=23 a=1,\ r=\tfrac23 and ∣r∣<1 |r|<1 :

11−23=3. \frac{1}{1-\tfrac23}=3.
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