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AP Calculus BC

AP · College BoardCalculus BC46 則筆記,位於 10 個資料夾,220 KB

cookie 製作的 College Board AP Calculus BC 考試準備筆記,共 46 篇,分為 10 個部分,依照課程主題編排。

Notes for AP Calculus BC (College Board), in folders for the course's ten units in their order, from limits and differentiation through integration, differential equations and applications to parametric, polar and vector functions and infinite series. Each note has definitions, theorems with their conditions, methods and worked examples for one topic. Delete any folder or note you don't need once the notes are yours.

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內容

  • Limits and continuity
    • Limits and limit techniques7 KB
    • Continuity and the Intermediate Value Theorem5 KB
    • Infinite limits, limits at infinity and asymptotes4 KB
  • Differentiation: definition and fundamental properties
    • The derivative as a limit5 KB
    • Derivative rules6 KB
  • Composite, implicit and inverse functions
    • The chain rule4 KB
    • Implicit differentiation and higher-order derivatives5 KB
    • Derivatives of inverse functions and inverse trigonometric functions5 KB
  • Contextual applications of differentiation
    • Derivatives and rates of change in context5 KB
    • Related rates5 KB
    • Local linearity and linearization4 KB
    • L'Hospital's rule5 KB
  • Analytical applications of differentiation
    • The Mean Value Theorem and the Extreme Value Theorem5 KB
    • Increasing and decreasing functions and absolute extrema4 KB
    • Concavity, points of inflection and the second derivative test4 KB
    • Connecting a function with its derivatives, and implicitly defined curves5 KB
    • Optimization5 KB
  • Integration and accumulation of change
    • Accumulation of change and Riemann sums6 KB
    • The definite integral and its properties5 KB
    • The Fundamental Theorem of Calculus and accumulation functions5 KB
    • Antiderivatives and basic integration4 KB
    • Integration by substitution4 KB
    • Long division, completing the square and partial fractions5 KB
    • Integration by parts4 KB
    • Improper integrals4 KB
  • Differential equations
    • Differential equations, solutions and slope fields5 KB
    • Euler's method4 KB
    • Separation of variables4 KB
    • Exponential growth and decay and logistic models5 KB
  • Applications of integration
    • Average value, motion and accumulation in context6 KB
    • Area between curves4 KB
    • Volumes with known cross sections4 KB
    • Volumes of revolution5 KB
    • Arc length4 KB
  • Parametric equations, polar coordinates and vector-valued functions
    • Parametric equations: derivatives and arc length5 KB
    • Vector-valued functions and planar motion5 KB
    • Polar coordinates: derivatives and area6 KB
  • Infinite sequences and series
    • Series, partial sums and geometric series4 KB
    • The nth term test, the integral test and p-series5 KB
    • Comparison tests5 KB
    • The alternating series test and its error bound4 KB
    • The ratio test and absolute and conditional convergence5 KB
    • Taylor polynomials5 KB
    • The Lagrange error bound4 KB
    • Radius and interval of convergence of power series5 KB
    • Maclaurin series and representing functions as power series6 KB

第一則筆記

Limits and continuity / Limits and limit techniques

What a limit says

The limit of f(x)f(x) as xx approaches cc is the number RR that f(x)f(x) can be made arbitrarily close to by taking xx sufficiently close to cc, without letting xx equal cc. It is written

lim⁡x→cf(x)=R. \lim_{x \to c} f(x) = R.

The value of ff at cc plays no part. The function may be undefined at cc, or defined with a different value, and the limit is still decided only by what happens nearby. That is why limits are the tool for describing the behaviour of x2−9x−3\frac{x^2 - 9}{x - 3} at x=3x = 3, where the expression itself is not defined.

A limit is a real number or it does not exist. Writing lim⁡x→cf(x)=∞\lim_{x \to c} f(x) = \infty describes the way in which a limit fails to exist, and it is not a value.

One-sided limits

lim⁡x→c−f(x)\lim_{x \to c^-} f(x) is the limit as xx approaches cc from the left, using only values below cc. lim⁡x→c+f(x)\lim_{x \to c^+} f(x) uses only values above cc. The two-sided limit exists exactly when both one-sided limits exist and are equal:

lim⁡x→cf(x)=R  ⟺  lim⁡x→c−f(x)=R and lim⁡x→c+f(x)=R. \lim_{x \to c} f(x) = R \iff \lim_{x \to c^-} f(x) = R \text{ and } \lim_{x \to c^+} f(x) = R.

For f(x)=2x−1f(x) = 2x - 1 when x<3x < 3 and f(x)=x2−6f(x) = x^2 - 6 when x≥3x \ge 3, the left limit at 33 is 2(3)−1=52(3) - 1 = 5 and the right limit is 9−6=39 - 6 = 3. They differ, so lim⁡x→3f(x)\lim_{x \to 3} f(x) does not exist, even though f(3)=3f(3) = 3 is defined.

Ways a limit can fail to exist

There are three common reasons.

  • The one-sided limits exist but are different, as in the jump above. A graph shows this as a break with the two sides ending at different heights.
  • The function is unbounded near cc. For 1x\frac{1}{x} at 00 the values grow without bound on the right and fall without bound on the left.
  • The function oscillates without settling. sin⁡(1x)\sin\left(\frac{1}{x}\right) as x→0x \to 0 swings between −1-1 and 11 infinitely often however close xx gets to 00, so no single value is approached.

Estimating limits from graphs and tables

On a graph, follow the curve towards x=cx = c from each side and read the height it is heading for. An open circle at x=cx = c means the function is not defined or takes a different value there, and the limit is the height of the hole. A graph drawn at a fixed scale can hide behaviour, such as a very fast oscillation or a narrow spike, so a graph supports an estimate and does not prove one.

From a table, choose values of xx closer and closer to cc on both sides and watch the outputs. For ex−1x\frac{e^x - 1}{x} near 00:

xx−0.01-0.01−0.001-0.0010.0010.0010.010.01
ex−1x\frac{e^x - 1}{x}0.995020.995020.999500.999501.000501.000501.005021.00502

The outputs close in on 11 from both sides, so the limit is estimated as 11. A table with values from only one side can only estimate the one-sided limit. A trend across a few values is evidence and not a guarantee.

Limit laws

If lim⁡x→cf(x)=L\lim_{x \to c} f(x) = L and lim⁡x→cg(x)=M\lim_{x \to c} g(x) = M both exist as real numbers, then

lim⁡x→c[f(x)±g(x)]=L±Mlim⁡x→c[k f(x)]=kLlim⁡x→c[f(x) g(x)]=LMlim⁡x→cf(x)g(x)=LM(M≠0). \begin{aligned} \lim_{x \to c} \left[ f(x) \pm g(x) \right] &= L \pm M \\ \lim_{x \to c} \left[ k\, f(x) \right] &= kL \\ \lim_{x \to c} \left[ f(x)\, g(x) \right] &= LM \\ \lim_{x \to c} \frac{f(x)}{g(x)} &= \frac{L}{M} \quad (M \ne 0). \end{aligned}

For a composite function, lim⁡x→cf(g(x))=f(lim⁡x→cg(x))\lim_{x \to c} f(g(x)) = f\left(\lim_{x \to c} g(x)\right) when ff is continuous at that limit of gg. Polynomials, rational functions (where the denominator is not zero), xn\sqrt[n]{x}, sin⁡x\sin x, cos⁡x\cos x, exe^x and ln⁡x\ln x are continuous on their domains, so their limits at a point of the domain are found by substituting. For instance lim⁡x→2x2+1x+3=55=1\lim_{x \to 2} \frac{x^2 + 1}{x + 3} = \frac{5}{5} = 1.

When substitution gives 00\frac{0}{0}

Substituting x=cx = c can give 00\frac{0}{0}. This is an indeterminate form and says nothing about the limit yet: the expression has to be rewritten first. The rewriting works because limits ignore the value at cc itself, so a common factor that vanishes at cc can be cancelled.

Factoring
lim⁡x→3x2−9x−3=lim⁡x→3(x−3)(x+3)x−3=lim⁡x→3(x+3)=6. \lim_{x \to 3} \frac{x^2 - 9}{x - 3} = \lim_{x \to 3} \frac{(x - 3)(x + 3)}{x - 3} = \lim_{x \to 3} (x + 3) = 6.
Multiplying by a conjugate

When a square root sits in the numerator or denominator, multiplying the top and bottom by the conjugate removes it:

lim⁡x→0x+4−2x=lim⁡x→0(x+4−2)(x+4+2)x(x+4+2)=lim⁡x→0xx(x+4+2)=lim⁡x→01x+4+2=14. \begin{aligned} \lim_{x \to 0} \frac{\sqrt{x + 4} - 2}{x} &= \lim_{x \to 0} \frac{\left(\sqrt{x + 4} - 2\right)\left(\sqrt{x + 4} + 2\right)}{x\left(\sqrt{x + 4} + 2\right)} \\ &= \lim_{x \to 0} \frac{x}{x\left(\sqrt{x + 4} + 2\right)} \\ &= \lim_{x \to 0} \frac{1}{\sqrt{x + 4} + 2} = \frac{1}{4}. \end{aligned}
Combining fractions
lim⁡x→01x+2−12x=lim⁡x→02−(x+2)2(x+2)x=lim⁡x→0−x2x(x+2)=lim⁡x→0−12(x+2)=−14. \lim_{x \to 0} \frac{\frac{1}{x + 2} - \frac{1}{2}}{x} = \lim_{x \to 0} \frac{\frac{2 - (x + 2)}{2(x + 2)}}{x} = \lim_{x \to 0} \frac{-x}{2x(x + 2)} = \lim_{x \to 0} \frac{-1}{2(x + 2)} = -\frac{1}{4}.
Trigonometric identities

Two limits are used repeatedly:

lim⁡x→0sin⁡xx=1,lim⁡x→01−cos⁡xx=0. \lim_{x \to 0} \frac{\sin x}{x} = 1, \qquad \lim_{x \to 0} \frac{1 - \cos x}{x} = 0.

They extend to other multiples of the variable by rescaling. For lim⁡x→0sin⁡3xx\lim_{x \to 0} \frac{\sin 3x}{x}, write sin⁡3xx=3⋅sin⁡3x3x\frac{\sin 3x}{x} = 3 \cdot \frac{\sin 3x}{3x}, and since 3x→03x \to 0 as x→0x \to 0, the limit is 3⋅1=33 \cdot 1 = 3.

If substitution gives a nonzero number over zero, such as 50\frac{5}{0}, the expression is not indeterminate. The function is unbounded near cc and the limit is either infinite or does not exist.

The squeeze theorem

If g(x)≤f(x)≤h(x)g(x) \le f(x) \le h(x) for all xx near cc (except possibly at cc), and lim⁡x→cg(x)=lim⁡x→ch(x)=L\lim_{x \to c} g(x) = \lim_{x \to c} h(x) = L, then lim⁡x→cf(x)=L\lim_{x \to c} f(x) = L.

It is used when the function is trapped between two simpler ones. To find lim⁡x→0x2sin⁡(1x)\lim_{x \to 0} x^2 \sin\left(\frac{1}{x}\right), note that −1≤sin⁡(1x)≤1-1 \le \sin\left(\frac{1}{x}\right) \le 1 for x≠0x \ne 0, and multiplying by x2≥0x^2 \ge 0 gives

−x2≤x2sin⁡(1x)≤x2. -x^2 \le x^2 \sin\left(\frac{1}{x}\right) \le x^2.

Both −x2-x^2 and x2x^2 tend to 00 as x→0x \to 0, so the limit is 00. Without the factor x2x^2, sin⁡(1x)\sin\left(\frac{1}{x}\right) has no limit at 00, so the squeeze is what tames the oscillation.

The two trigonometric limits above are themselves proved by squeezing, using a comparison of areas in a unit circle.

Choosing a method

Try substitution first. If the result is a number, it is the limit, provided the function is continuous there. If it is 00\frac{0}{0}, look for a factor to cancel, a conjugate to multiply by, a fraction to combine or a trigonometric identity to apply. If the expression involves a bounded oscillating factor multiplied by something that tends to zero, consider the squeeze theorem. For piecewise functions, or at a point where the formula changes, work out each one-sided limit separately. Where the form is 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} and the expression is differentiable, L'Hospital's rule gives another route once derivatives are available.

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