AP® Calculus BC

Formulas and theorems to know

The exam gives no formula sheet. These are the formulas and theorems to know by heart, what each is for and when to use it.

Three habits that save points

Limits and continuity

FormulaWhat it isWhen you use itLearn it in
limx→cf(x)\lim_{x \to c} f(x)=f(c)= f(c)Continuity at x=cx = c: f(c)f(c) is defined, the limit exists, and the two are equal.To show a function is continuous at a point. For a piecewise function, find both one-sided limits first.Unit 1
Continuity at a PointPractice it: Limit explorer
limx→0sin⁡xx\lim_{x \to 0} \frac{\sin x}{x}=1= 1A special limit, with xx in radians, found with the squeeze theorem.Limits such as limx→0sin⁡(3x)x\lim_{x \to 0} \frac{\sin(3x)}{x}: rewrite as 3⋅sin⁡(3x)3x3 \cdot \frac{\sin(3x)}{3x}.Unit 1
The Squeeze TheoremPractice it: Limit explorer
limx→01−cos⁡xx\lim_{x \to 0} \frac{1 - \cos x}{x}=0= 0The companion special limit, also with xx in radians.Limits with 1−cos⁡x1 - \cos x over xx; together with the first, it gives the derivatives of sine and cosine.Unit 1
The Squeeze Theorem
g(x)≤f(x)≤h(x)g(x) \le f(x) \le h(x)⇒limx→cf(x)\Rightarrow \lim_{x \to c} f(x)=L= LThe squeeze theorem, when g(x)≤f(x)≤h(x)g(x) \le f(x) \le h(x) near cc and gg and hh both have limit LL at cc.When ff is trapped between two functions with the same limit, such as a bounded factor like sin⁡1x\sin\frac{1}{x} times something that goes to 0.Unit 1
The Squeeze TheoremPractice it: Limit explorer
f(c)f(c)=dfor somecin[a,b]= d \ \text{for some}\ c \ \text{in}\ [a, b]The Intermediate Value Theorem, when ff is continuous on [a,b][a, b] and dd is between f(a)f(a) and f(b)f(b).To show an equation f(x)=df(x) = d has a solution. Say first why ff is continuous on the closed interval.Unit 1
The Intermediate Value Theorem
limx→cf(x)g(x)\lim_{x \to c} \frac{f(x)}{g(x)}=limx→cf′(x)g′(x)= \lim_{x \to c} \frac{f'(x)}{g'(x)}L'Hospital's rule, when ff and gg both have limit 0, or both have infinite limits, and the limit on the right exists.For 00\frac{0}{0} and ∞∞\frac{\infty}{\infty} forms. Write the two limits separately first, then differentiate top and bottom on their own (not the quotient rule).Unit 4
L'Hospital's Rule

Derivative rules

FormulaWhat it isWhen you use itLearn it in
f′(a)f'(a)=limh→0f(a+h)−f(a)h= \lim_{h \to 0} \frac{f(a + h) - f(a)}{h}The definition of the derivative: the limit of the slopes of secant lines.To recognize a limit as a derivative in disguise, or to check differentiability where two pieces meet.Unit 2
The Derivative and Its NotationPractice it: Tangent tracer
f(b)−f(a)b−a\frac{f(b) - f(a)}{b - a}The average rate of change of ff on [a,b][a, b], the slope of a secant line.Rates over an interval from a formula or a table; to estimate f′(c)f'(c) from a table, use the two values closest to cc on either side.Unit 2
Average and Instantaneous Rates of ChangePractice it: Tangent tracer
ddxxn=nxn−1\frac{d}{dx} x^n = n x^{n - 1}The power rule, for any real number nn.Powers, roots and reciprocals. Rewrite x\sqrt{x} as x1/2x^{1/2} and 1x2\frac{1}{x^2} as x−2x^{-2} first.Unit 2
The Power RulePractice it: Rule drills
ddx[f(x)g(x)]\frac{d}{dx}\left[f(x)g(x)\right]=f′(x)g(x)= f'(x)g(x)+f(x)g′(x)+ f(x)g'(x)The product rule, for a product of two functions.A product of two functions of xx; for three factors, use it twice.Unit 2
The Product RulePractice it: Rule drills
ddx[f(x)g(x)]\frac{d}{dx}\left[\frac{f(x)}{g(x)}\right]=f′(x)g(x)−f(x)g′(x)[g(x)]2= \frac{f'(x)g(x) - f(x)g'(x)}{\left[g(x)\right]^2}The quotient rule, for a quotient of two functions.A quotient that does not simplify by dividing first. The order on top matters.Unit 2
The Quotient RulePractice it: Rule drills
ddxsin⁡x\frac{d}{dx}\sin x=cos⁡x,= \cos x,ddxcos⁡x\quad \frac{d}{dx}\cos x=−sin⁡x= -\sin xDerivatives of sine and cosine, with xx in radians.Every trigonometric derivative starts here. The minus sign belongs to cosine.Unit 2
Derivatives of sin x, cos x, e to the x and ln xPractice it: Rule drills
ddxex\frac{d}{dx}e^x=ex,= e^x,ddxln⁡x\quad \frac{d}{dx}\ln x=1x= \frac{1}{x}Derivatives of the natural exponential and the natural logarithm.Exponentials and logarithms. With the chain rule, ddxeu=euu′\frac{d}{dx}e^{u} = e^{u}u' and ddxln⁡u=u′u\frac{d}{dx}\ln u = \frac{u'}{u}.Unit 2
Derivatives of sin x, cos x, e to the x and ln xPractice it: Rule drills
ddxtan⁡x\frac{d}{dx}\tan x=sec2⁡x,= \sec^2 x,ddxsec⁡x\quad \frac{d}{dx}\sec x=sec⁡xtan⁡x= \sec x \tan xDerivatives of tangent and secant, from the quotient rule.Tangent and secant directly, without rewriting them as quotients each time.Unit 2
Derivatives of tan, cot, sec and csc
ddxcot⁡x\frac{d}{dx}\cot x=−csc2⁡x,= -\csc^2 x,ddxcsc⁡x\quad \frac{d}{dx}\csc x=−csc⁡xcot⁡x= -\csc x \cot xDerivatives of cotangent and cosecant.The co-functions follow the same pattern as tangent and secant, with minus signs.Unit 2
Derivatives of tan, cot, sec and csc
ddxf(g(x))\frac{d}{dx}f(g(x))=f′(g(x))⋅g′(x)= f'(g(x)) \cdot g'(x)The chain rule, for a composite function.Any function inside another, such as e3xe^{3x}, sin⁡(x2)\sin(x^2) or (2x+1)5(2x + 1)^5: multiply by the derivative of the inside.Unit 3
The Chain RulePractice it: Rule drills
ddx[yn]\frac{d}{dx}\left[y^n\right]=nyn−1dydx= n y^{n - 1}\frac{dy}{dx}Implicit differentiation: yy is a function of xx, so the chain rule brings out dydx\frac{dy}{dx}.Curves such as x2+xy+y2=7x^2 + xy + y^2 = 7: differentiate both sides, keep the =0= 0, then solve for dydx\frac{dy}{dx}.Unit 3
Implicit DifferentiationPractice it: Rule drills
(f−1)′(b)\left(f^{-1}\right)'(b)=1f′(a)wheref(a)= \frac{1}{f'(a)} \ \text{where}\ f(a)=b= bThe derivative of an inverse function at a point.When you know ff but not its inverse: find the input aa with f(a)=bf(a) = b first.Unit 3
Derivatives of Inverse Functions
ddxarcsin⁡x\frac{d}{dx}\arcsin x=11−x2,= \frac{1}{\sqrt{1 - x^2}},ddxarctan⁡x\quad \frac{d}{dx}\arctan x=11+x2= \frac{1}{1 + x^2}Derivatives of inverse sine and inverse tangent.Inverse trigonometric functions, with the chain rule for arcsin⁡u\arcsin u and arctan⁡u\arctan u.Unit 3
Derivatives of Inverse Trigonometric Functions
y=f(a)+f′(a)(x−a)y = f(a) + f'(a)(x - a)The tangent line at x=ax = a, in point-slope form.Tangent lines and local linear approximation. Whether the estimate is too big or too small comes from concavity.Unit 4
Local Linearity and LinearizationPractice it: Tangent tracer

Theorems and curve analysis

FormulaWhat it isWhen you use itLearn it in
differentiable atc\text{differentiable at}\ c⇒continuous atc\Rightarrow \text{continuous at}\ cDifferentiability implies continuity. Not the other way: |x||x| is continuous at 0 but not differentiable there.To supply the continuity a theorem needs when you are told only that ff is differentiable.Unit 2
Differentiability and Continuity
f′(c)f'(c)=f(b)−f(a)b−a,= \frac{f(b) - f(a)}{b - a},a<c<b\ a < c < bThe Mean Value Theorem, when ff is continuous on [a,b][a, b] and differentiable on (a,b)(a, b).To show an instantaneous rate equals an average rate. State both hypotheses in words first.Unit 5
The Mean Value TheoremPractice it: Curve analyzer
max[a,b]⁡fandmin[a,b]⁡fexist\max_{[a, b]} f \ \text{and}\ \min_{[a, b]} f \ \text{exist}The Extreme Value Theorem, when ff is continuous on the closed interval [a,b][a, b].To know absolute extrema exist before you look for them. It needs a closed interval and continuity.Unit 5
Extreme Value Theorem, Global and Local Extrema, Critical Points
f′>0f' > 0⇒fincreasing,\Rightarrow f \ \text{increasing},f′<0\quad f' < 0⇒fdecreasing\Rightarrow f \ \text{decreasing}Increasing and decreasing from the sign of f′f'.Where ff rises or falls, from a formula, a table, or a graph of f′f'.Unit 5
Where a Function Increases or DecreasesPractice it: Curve analyzer
f′from+to−atcf' \ \text{from}\ + \ \text{to}\ - \ \text{at}\ c⇒relative max\Rightarrow \text{relative max}The first derivative test. From negative to positive: a relative minimum.Any relative extremum. Name the function that changes sign and say from what to what; f′(c)=0f'(c) = 0 alone is not enough.Unit 5
The First Derivative TestPractice it: Curve analyzer
comparef(a),\text{compare}\ f(a),f(b),\ f(b),f(each critical point)\ f(\text{each critical point})The candidates test for absolute extrema on [a,b][a, b], also called the closed interval method.An absolute (global) maximum or minimum on a closed interval. A sign change only shows a relative extremum.Unit 5
The Candidates TestPractice it: Curve analyzer
f″>0f'' > 0⇒concave up,\Rightarrow \text{concave up},f″<0\quad f'' < 0⇒concave down\Rightarrow \text{concave down}Concavity. A point of inflection is where f″f'' changes sign (where f′f' changes from increasing to decreasing, or back).Concavity and inflection points, and whether a tangent line estimate is an overestimate (concave down) or an underestimate (concave up).Unit 5
Concavity and Points of InflectionPractice it: Curve analyzer
f′(c)f'(c)=0,= 0,f″(c)<0\ f''(c) < 0⇒relative max\Rightarrow \text{relative max}The second derivative test. If f″(c)>0f''(c) > 0, a relative minimum; if f″(c)=0f''(c) = 0, the test says nothing.A relative extremum at a critical point where f″f'' is easy to evaluate.Unit 5
The Second Derivative TestPractice it: Curve analyzer

Integrals and the Fundamental Theorem

FormulaWhat it isWhen you use itLearn it in
∫xndx\int x^n\,dx=xn+1n+1= \frac{x^{n + 1}}{n + 1}+C+ C(n≠−1)\quad (n \ne -1)The power rule for antiderivatives.Powers and roots, rewritten as powers first. Check by differentiating.Unit 6
Antiderivatives and Indefinite Integrals
∫1xdx=ln⁡|x|+C\int \frac{1}{x}\,dx = \ln|x| + CThe case n=−1n = -1, with the absolute value.An integrand 1x\frac{1}{x}, or u′u\frac{u'}{u} after a substitution.Unit 6
Antiderivatives and Indefinite Integrals
∫exdx=ex+C\int e^x\,dx = e^x + CThe antiderivative of the natural exponential.Exponentials; with a substitution, ∫ekxdx=1kekx+C\int e^{kx}\,dx = \frac{1}{k}e^{kx} + C.Unit 6
Antiderivatives and Indefinite Integrals
∫sin⁡xdx\int \sin x\,dx=−cos⁡x= -\cos x+C,+ C,∫cos⁡xdx\quad \int \cos x\,dx=sin⁡x= \sin x+C+ CAntiderivatives of sine and cosine.Trigonometric integrands. The minus sign is on the antiderivative of sine.Unit 6
Antiderivatives and Indefinite Integrals
∫sec2⁡xdx\int \sec^2 x\,dx=tan⁡x= \tan x+C,+ C,∫sec⁡xtan⁡xdx\quad \int \sec x \tan x\,dx=sec⁡x= \sec x+C+ CThe derivatives of tangent and secant, read backward.Integrands that are exactly one of these derivatives.Unit 6
Antiderivatives and Indefinite Integrals
∫11−x2dx\int \frac{1}{\sqrt{1 - x^2}}\,dx=arcsin⁡x= \arcsin x+C,+ C,∫11+x2dx\quad \int \frac{1}{1 + x^2}\,dx=arctan⁡x= \arctan x+C+ CThe inverse trigonometric derivatives, read backward.Integrands of these forms, sometimes after a substitution or after completing the square.Unit 6
Antiderivatives and Indefinite Integrals
∫abf(x)dx\int_a^b f(x)\,dx=limn→∞∑i=1nf(xi)Δx,= \lim_{n \to \infty}\sum_{i=1}^{n} f(x_i)\Delta x,Δx\quad \Delta x=b−an= \frac{b - a}{n}The definite integral as a limit of Riemann sums.To recognize a limit of sums as an integral: read Δx\Delta x and xix_i to find aa, bb and ff.Unit 6
Riemann Sums, Sigma Notation and the Definite IntegralPractice it: Riemann sums
Δx12[f(x0)+f(x1)]\frac{\Delta x_1}{2}\left[f(x_0) + f(x_1)\right]+Δx22[f(x1)+f(x2)]+ \frac{\Delta x_2}{2}\left[f(x_1) + f(x_2)\right]+⋯+ \cdotsThe trapezoidal sum, each trapezoid with its own width.Approximating an integral from a table. Widths may differ; never assume they are equal.Unit 6
Estimating Area with Riemann SumsPractice it: Riemann sums
ddx∫axf(t)dt\frac{d}{dx}\int_a^x f(t)\,dt=f(x)= f(x)The Fundamental Theorem of Calculus, first part, for continuous ff.Derivatives of accumulation functions. With an upper limit g(x)g(x), multiply by g′(x)g'(x): ddx∫ag(x)f(t)dt\frac{d}{dx}\int_a^{g(x)} f(t)\,dt=f(g(x))g′(x)= f(g(x))g'(x).Unit 6
The Fundamental Theorem and Accumulation FunctionsPractice it: Accumulation
∫abf(x)dx\int_a^b f(x)\,dx=F(b)−F(a),= F(b) - F(a),whereF′\ \text{where}\ F'=f= fThe Fundamental Theorem of Calculus, second part: evaluate with any antiderivative.Definite integrals without a calculator.Unit 6
The Fundamental Theorem and Definite IntegralsPractice it: Accumulation
∫baf(x)dx\int_b^a f(x)\,dx=−∫abf(x)dx= -\int_a^b f(x)\,dxReversing the limits changes the sign.An accumulation function evaluated below its lower limit, such as ∫41f(t)dt\int_4^1 f(t)\,dt.Unit 6
Properties of Definite IntegralsPractice it: Accumulation
∫abf(x)dx\int_a^b f(x)\,dx+∫bcf(x)dx+ \int_b^c f(x)\,dx=∫acf(x)dx= \int_a^c f(x)\,dxIntegrals over adjacent intervals add.Integrals given in pieces, or a graph made of pieces whose areas you add.Unit 6
Properties of Definite IntegralsPractice it: Accumulation
∫f(g(x))g′(x)dx\int f(g(x))g'(x)\,dx=∫f(u)du,= \int f(u)\,du,u\quad u=g(x)= g(x)Substitution: the chain rule run backward.An inside function whose derivative, up to a constant, is also a factor. For a definite integral, change the limits too.Unit 6
Integrating by Substitution
∫udv=uv−∫vdu\int u\,dv = uv - \int v\,duIntegration by parts, the product rule run backward.A product such as xexx e^x, xsin⁡xx\sin x or ln⁡x\ln x: choose uu to get simpler when differentiated. For a definite integral, evaluate uvuv at both limits.Unit 6
Integration by PartsPractice it: Integration methods
Ax−a+Bx−b\frac{A}{x - a} + \frac{B}{x - b}Partial fractions for p(x)(x−a)(x−b)\frac{p(x)}{(x - a)(x - b)} with distinct linear factors (divide first if the top has the same or higher degree).A rational function whose denominator factors into distinct linear factors; each piece integrates to a logarithm.Unit 6
Linear Partial FractionsPractice it: Integration methods
∫a∞f(x)dx\int_a^{\infty} f(x)\,dx=limb→∞∫abf(x)dx= \lim_{b \to \infty} \int_a^b f(x)\,dxAn improper integral, defined as a limit; it converges when the limit is a finite number.An infinite limit of integration, or an integrand that is unbounded at an endpoint. Keep the limit notation to the end; never substitute ∞\infty.Unit 6
Improper IntegralsPractice it: Integration methods

Motion, rates and accumulation

FormulaWhat it isWhen you use itLearn it in
v(t)v(t)=x′(t),= x'(t),a(t)\quad a(t)=v′(t)= v'(t)=x″(t)= x''(t)Velocity and acceleration from position.Particle motion on a line.Unit 4
Straight-Line Motion: Position, Velocity, AccelerationPractice it: Motion lab
v,asame signv, a \ \text{same sign}⇒speeding up\Rightarrow \text{speeding up}Speeding up or slowing down. Opposite signs: slowing down. Speed is |v(t)||v(t)|.Any speeding-up question: give the signs of both vv and aa at that time.Unit 4
Straight-Line Motion: Position, Velocity, AccelerationPractice it: Motion lab
ddt[x2+y2]\frac{d}{dt}\left[x^2 + y^2\right]=2xdxdt+2ydydt= 2x\frac{dx}{dt} + 2y\frac{dy}{dt}Related rates: differentiate the equation that links the quantities with respect to time.Ladders, cones, shadows: differentiate first, then substitute the values at the moment asked about.Unit 4
Introduction to Related RatesPractice it: Related rates
favgf_{\text{avg}}=1b−a∫abf(x)dx= \frac{1}{b - a}\int_a^b f(x)\,dxThe average value of ff on [a,b][a, b]."Average temperature" or "average velocity" asks for the average value of the function, not its average rate of change.Unit 8
Average Value of a Function
x(t)x(t)=x(t0)= x(t_0)+∫t0tv(s)ds+ \int_{t_0}^{t} v(s)\,dsPosition from velocity and a known position.Position at a time: start from the time where the position is known, not always t=0t = 0.Unit 8
Motion with IntegralsPractice it: Motion lab
∫abv(t)dtand∫ab|v(t)|dt\int_a^b v(t)\,dt \ \text{and}\ \int_a^b |v(t)|\,dtDisplacement (the first) and total distance traveled (the second).Total distance: integrate the speed, or, without a calculator, split where vv changes sign.Unit 8
Motion with IntegralsPractice it: Motion lab
A(t)A(t)=A(0)= A(0)+∫0tr(s)ds+ \int_0^t r(s)\,dsAn amount from a rate and a starting amount (net change).Water in a tank, people in a park: keep the starting amount, and subtract the rate out from the rate in.Unit 8
Accumulation in ContextPractice it: Accumulation

Differential equations

FormulaWhat it isWhen you use itLearn it in
dydx\frac{dy}{dx}=f(x)g(y)= f(x)g(y)⇒∫1g(y)dy\Rightarrow \int \frac{1}{g(y)}\,dy=∫f(x)dx= \int f(x)\,dxSeparation of variables.A particular solution: add +C+ C as you antidifferentiate, use the initial condition right away, then solve for yy.Unit 7
General Solutions by Separation of VariablesPractice it: Slope fields
dydt=ky⇒y=y0ekt\frac{dy}{dt} = ky \Rightarrow y = y_0 e^{kt}Exponential growth (k>0k > 0) and decay (k<0k < 0); y0y_0 is the value at t=0t = 0.A rate proportional to the amount present.Unit 7
Exponential ModelsPractice it: Slope fields
yn+1y_{n+1}=yn= y_n+Δx⋅dydx|(xn,yn)+ \Delta x \cdot \frac{dy}{dx}\Big|_{(x_n,\, y_n)}Euler's method: step along the tangent line with the slope at the current point.Approximating a solution value from a differential equation and a starting point. Concave up: the steps land below the curve (underestimate); concave down: above.Unit 7
Euler's MethodPractice it: Euler and logistic
dPdt=kP(1−PL)\frac{dP}{dt} = kP\left(1 - \frac{P}{L}\right)Logistic growth with carrying capacity LL and k>0k > 0.P→LP \to L as t→∞t \to \infty for P(0)>0P(0) > 0; PP grows fastest when P=L2P = \frac{L}{2}.Unit 7
Logistic ModelsPractice it: Euler and logistic

Area and volume

FormulaWhat it isWhen you use itLearn it in
∫ab[f(x)−g(x)]dx\int_a^b \left[f(x) - g(x)\right]dxArea between curves, ff above gg, slicing along xx.Area between two graphs. Split at crossings if the top curve changes.Unit 8
Area Between Curves (Functions of x)Practice it: Area and volume
∫cd[p(y)−q(y)]dy\int_c^d \left[p(y) - q(y)\right]dyArea slicing along yy: the right curve minus the left curve.When the region is easier to describe with xx as a function of yy.Unit 8
Area Between Curves (Functions of y)Practice it: Area and volume
∫abA(x)dx,\int_a^b A(x)\,dx,A\quad A=s2for squares= s^2 \ \text{for squares}Volume from cross sections of area A(x)A(x); a square of side ss has area s2s^2.Known cross sections on a base region: the side ss is the length across the base at xx.Unit 8
Volumes with Square and Rectangle Cross SectionsPractice it: Area and volume
AA=34s2,= \frac{\sqrt{3}}{4}s^2,A\quad A=π8s2,= \frac{\pi}{8}s^2,A\quad A=12s2= \frac{1}{2}s^2Cross-section areas: an equilateral triangle of side ss, a semicircle of diameter ss, an isosceles right triangle with a leg ss in the base.Triangle and semicircle cross sections; with the hypotenuse ss in the base, the right triangle has area 14s2\frac{1}{4}s^2.Unit 8
Volumes with Triangle and Semicircle Cross SectionsPractice it: Area and volume
π∫ab[R(x)]2dx\pi\int_a^b \left[R(x)\right]^2 dxThe disc method, with the radius RR measured from the axis of revolution.A region that touches the axis. About a line y=ky = k, the radius is |f(x)−k||f(x) - k|.Unit 8
Disc Method About the AxesPractice it: Area and volume
π∫ab([R(x)]2−[r(x)]2)dx\pi\int_a^b \left(\left[R(x)\right]^2 - \left[r(x)\right]^2\right)dxThe washer method: outer radius RR and inner radius rr, both from the axis.A region with a gap from the axis. Square each radius on its own; (R−r)2(R - r)^2 is wrong.Unit 8
Washer Method About the AxesPractice it: Area and volume
∫ab1+(f′(x))2dx\int_a^b \sqrt{1 + \left(f'(x)\right)^2}\,dxThe length of the graph of y=f(x)y = f(x) from x=ax = a to x=bx = b.Arc length of a function's graph; for a curve given by x=g(y)x = g(y), use 1+(g′(y))2dy\sqrt{1 + \left(g'(y)\right)^2}\,dy.Unit 8
Arc Length and Distance Traveled

Parametric, vector and polar

FormulaWhat it isWhen you use itLearn it in
dydx\frac{dy}{dx}=dy/dtdx/dt,= \frac{dy/dt}{dx/dt},dxdt≠0\quad \frac{dx}{dt} \ne 0The slope of a parametric curve.Tangent lines: horizontal where dydt=0\frac{dy}{dt} = 0 and dxdt≠0\frac{dx}{dt} \ne 0; vertical where dxdt=0\frac{dx}{dt} = 0 and dydt≠0\frac{dy}{dt} \ne 0.Unit 9
Parametric Equations and Their DerivativesPractice it: Parametric motion
d2ydx2\frac{d^2y}{dx^2}=ddt(dydx)dx/dt= \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{dx/dt}The second derivative of a parametric curve.Concavity of a parametric curve. Divide by dxdt\frac{dx}{dt} again; the derivative of dydx\frac{dy}{dx} with respect to tt is not enough.Unit 9
Second Derivatives of Parametric EquationsPractice it: Parametric motion
∫ab(x′(t))2+(y′(t))2dt\int_a^b \sqrt{\left(x'(t)\right)^2 + \left(y'(t)\right)^2}\,dtArc length of a parametric curve, and the distance a particle travels.Distance traveled in the plane: integrate the speed.Unit 9
Arc Length of a Parametric CurvePractice it: Parametric motion
|v(t)|\left|\mathbf{v}(t)\right|=(x′(t))2+(y′(t))2= \sqrt{\left(x'(t)\right)^2 + \left(y'(t)\right)^2}Speed, the length of the velocity vector v(t)=⟨x′(t),y′(t)⟩\mathbf{v}(t) = \left\langle x'(t), y'(t) \right\rangle.Speed of a particle in the plane. It is a magnitude; dydx\frac{dy}{dx} is the slope of the path, not the speed.Unit 9
Motion in the PlanePractice it: Parametric motion
x(b)x(b)=x(a)= x(a)+∫abx′(t)dt+ \int_a^b x'(t)\,dtPosition from velocity, one component at a time.The position at a later time: add the known position to the integral of each velocity component.Unit 9
Integrating Vector-Valued FunctionsPractice it: Parametric motion
x=rcos⁡θ,y=rsin⁡θx = r\cos\theta, \quad y = r\sin\thetaFrom polar to rectangular coordinates.Every polar derivative starts here: dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta} with rr a function of θ\theta.Unit 9
Polar Coordinates and Polar DerivativesPractice it: Polar lab
12∫αβr2dθ\frac{1}{2}\int_{\alpha}^{\beta} r^2\,d\thetaThe area swept by a polar curve from θ=α\theta = \alpha to θ=β\theta = \beta.Polar area. Square rr, keep the 12\frac{1}{2}, and find the limits where the curve meets the origin (r=0r = 0) or another curve.Unit 9
Area Inside a Polar CurvePractice it: Polar lab
12∫αβ(R2−r2)dθ\frac{1}{2}\int_{\alpha}^{\beta} \left(R^2 - r^2\right)d\thetaThe area between an outer polar curve RR and an inner curve rr.Square each radius on its own; (R−r)2(R - r)^2 is wrong. The limits come from where the curves meet.Unit 9
Area Between Two Polar CurvesPractice it: Polar lab

Series tests

FormulaWhat it isWhen you use itLearn it in
∑n=0∞arn\sum_{n=0}^{\infty} ar^n=a1−r,= \frac{a}{1 - r},|r|<1\quad |r| < 1A geometric series: it converges when |r|<1|r| < 1 and diverges when |r|≥1|r| \ge 1.Sums of series with a constant ratio, and the comparison series for many tests.Unit 10
Geometric SeriesPractice it: Series lab
limn→∞an≠0\lim_{n \to \infty} a_n \ne 0⇒∑andiverges\Rightarrow \sum a_n \ \text{diverges}The nth term test, for divergence only.A first check. If the terms do approach 0, this test says nothing.Unit 10
The nth Term Test for DivergencePractice it: Series lab
∑n=1∞1npconverges whenp>1\sum_{n=1}^{\infty} \frac{1}{n^p} \ \text{converges when}\ p > 1The pp-series; with p=1p = 1 it is the harmonic series, which diverges.The comparison series for terms that behave like a power of nn.Unit 10
Harmonic Series and p-SeriesPractice it: Series lab
∑n=1∞anand∫1∞f(x)dx\sum_{n=1}^{\infty} a_n \ \text{and}\ \int_1^{\infty} f(x)\,dxThe integral test: both converge or both diverge, when an=f(n)a_n = f(n) with ff positive, continuous and decreasing.Terms that are a function you can integrate. State the three conditions on ff.Unit 10
The Integral TestPractice it: Series lab
0<limn→∞anbn<∞0 < \lim_{n \to \infty} \frac{a_n}{b_n} < \inftyThe limit comparison test, for positive terms: ∑an\sum a_n and ∑bn\sum b_n do the same thing. (Direct comparison: 0≤an≤bn0 \le a_n \le b_n and ∑bn\sum b_n converges, then ∑an\sum a_n converges.)Terms that look like a geometric or pp-series for large nn. Name the comparison series and why it converges or diverges.Unit 10
Comparison TestsPractice it: Series lab
∑(−1)nan,\sum (-1)^n a_n,andecreasing,\quad a_n \ \text{decreasing},an→0\ a_n \to 0The alternating series test: then the series converges.Series whose signs alternate. Check both conditions in words; the test never shows divergence.Unit 10
The Alternating Series TestPractice it: Series lab
LL=limn→∞|an+1an|= \lim_{n \to \infty} \left|\frac{a_{n+1}}{a_n}\right|The ratio test: L<1L < 1 converges absolutely, L>1L > 1 diverges, L=1L = 1 decides nothing.Terms with factorials or powers such as 3n3^n, and the radius of a power series. At the endpoints of a power series L=1L = 1, so test them another way.Unit 10
The Ratio TestPractice it: Series lab
∑|an|converges\sum |a_n| \ \text{converges}⇒∑anconverges\Rightarrow \sum a_n \ \text{converges}Absolute convergence implies convergence. A series that converges but not absolutely converges conditionally.Series with mixed signs: test ∑|an|\sum |a_n| first.Unit 10
Absolute and Conditional ConvergencePractice it: Series lab

Taylor series and error bounds

FormulaWhat it isWhen you use itLearn it in
Pn(x)P_n(x)=∑k=0nf(k)(a)k!(x−a)k= \sum_{k=0}^{n} \frac{f^{(k)}(a)}{k!}(x - a)^kThe Taylor polynomial of degree nn for ff about x=ax = a (Maclaurin when a=0a = 0).Approximating ff near aa. A polynomial ends at its last term; a series goes on with +⋯+ \cdots or a general term.Unit 10
Taylor PolynomialsPractice it: Taylor lab
|S−Sn|≤an+1\left|S - S_n\right| \le a_{n+1}The alternating series error bound: the error is at most the size of the first term left out.An alternating series that meets the test's conditions. Say so before you use the bound.Unit 10
The Alternating Series Error BoundPractice it: Taylor lab
|f(x)−Pn(x)|≤M|x−a|n+1(n+1)!M=max⁡|f(n+1)(z)|\begin{aligned}&\left|f(x) - P_n(x)\right| \\ &\quad \le \frac{M\left|x - a\right|^{n+1}}{(n + 1)!} \\ &M = \max\left|f^{(n+1)}(z)\right|\end{aligned}The Lagrange error bound, where MM is the maximum of the next derivative taken for zz between aa and xx.The error of a Taylor polynomial when the series does not alternate, or when you know a bound on the next derivative.Unit 10
The Lagrange Error BoundPractice it: Taylor lab
11−x\frac{1}{1 - x}=∑n=0∞xn,= \sum_{n=0}^{\infty} x^n,|x|<1\quad |x| < 1The geometric series as a power series.Series for 11+x2\frac{1}{1 + x^2}, 12−x\frac{1}{2 - x} and others by substitution; integrate it to reach ln⁡(1+x)\ln(1 + x) and arctan⁡x\arctan x.Unit 10
Taylor and Maclaurin SeriesPractice it: Taylor lab
exe^x=∑n=0∞xnn!= \sum_{n=0}^{\infty} \frac{x^n}{n!}The Maclaurin series for exe^x, for every real xx.With substitution: e−x2e^{-x^2}=1−x2+x42!−⋯= 1 - x^2 + \frac{x^4}{2!} - \cdots.Unit 10
Taylor and Maclaurin SeriesPractice it: Taylor lab
sin⁡x\sin x=∑n=0∞(−1)nx2n+1(2n+1)!,= \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{(2n + 1)!},cos⁡x\quad \cos x=∑n=0∞(−1)nx2n(2n)!= \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n}}{(2n)!}The Maclaurin series for sine and cosine, for every real xx.Odd powers for sine, even for cosine; each alternates, so the alternating series error bound often applies.Unit 10
Taylor and Maclaurin SeriesPractice it: Taylor lab
|x−a|<R\left|x - a\right| < RA power series centered at aa converges inside its radius RR; the endpoints x=a±Rx = a \pm R are tested one at a time.The interval of convergence: the ratio test gives RR, then each endpoint gets its own test. Radius and interval are different answers.Unit 10
Radius and Interval of ConvergencePractice it: Series lab
ddx∑cnxn\frac{d}{dx}\sum c_n x^n=∑ncnxn−1,= \sum n c_n x^{n-1},∫∑cnxndx\quad \int \sum c_n x^n\,dx=C= C+∑cnxn+1n+1+ \sum \frac{c_n x^{n+1}}{n + 1}A power series is differentiated and integrated term by term, with the same radius.New series from known ones. Check the endpoints again: they can change.Unit 10
Representing Functions as Power SeriesPractice it: Taylor lab

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