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GRE Mathematics Subject Test

Entrance · ETSMathematics21 catatan dalam 3 folder, 152 KB

21 catatan belajar untuk ETS Entrance Mathematics, dibuat oleh cookie, dalam 3 bagian yang mengikuti topik kursus.

Notes for the GRE Mathematics Subject Test, in three folders following ETS's published content list: calculus, algebra (elementary, linear and abstract algebra, and number theory) and additional topics (analysis, topology, complex variables, probability and statistics, discrete mathematics, numerical analysis). Each note has definitions, results and worked examples at undergraduate level.

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  • Calculus
    • Limits and continuity6 KB
    • Differentiation7 KB
    • Integration8 KB
    • Sequences and series7 KB
    • Multivariable and vector calculus8 KB
    • Differential equations7 KB
  • Algebra
    • Elementary algebra7 KB
    • Trigonometry and coordinate geometry6 KB
    • Matrices, determinants and systems of linear equations6 KB
    • Vector spaces and linear maps6 KB
    • Eigenvalues, diagonalisation and orthogonality7 KB
    • Group theory8 KB
    • Rings and modules7 KB
    • Field theory8 KB
    • Number theory6 KB
  • Additional topics
    • Real analysis7 KB
    • Topology8 KB
    • Complex variables9 KB
    • Probability and statistics8 KB
    • Discrete mathematics9 KB
    • Numerical analysis8 KB

Catatan pertama

Calculus / Limits and continuity

Limits

The statement lim⁡x→af(x)=L\lim_{x \to a} f(x) = L means that f(x)f(x) can be made as close to LL as we like by taking xx close enough to aa, without xx being equal to aa. The function need not be defined at aa, and even if it is, its value there plays no part in the limit. In the formal version, for every ε>0\varepsilon > 0 there is a δ>0\delta > 0 such that 0<∣x−a∣<δ0 < |x - a| < \delta implies ∣f(x)−L∣<ε|f(x) - L| < \varepsilon.

A one-sided limit approaches aa from one side only, written lim⁡x→a−\lim_{x \to a^-} and lim⁡x→a+\lim_{x \to a^+}. The two-sided limit exists exactly when both one-sided limits exist and are equal. For f(x)=∣x∣/xf(x) = |x|/x the left limit at 00 is −1-1 and the right limit is 11, so there is no limit at 00.

A limit at infinity describes behaviour as xx grows without bound, and an infinite limit means the values grow without bound. For a rational function, divide numerator and denominator by the highest power of xx in the denominator. For example

lim⁡x→∞3x2−x+52x2+7=lim⁡x→∞3−1/x+5/x22+7/x2=32. \lim_{x \to \infty} \frac{3x^2 - x + 5}{2x^2 + 7} = \lim_{x \to \infty} \frac{3 - 1/x + 5/x^2}{2 + 7/x^2} = \frac{3}{2}.
Limit laws

If lim⁡x→af(x)=L\lim_{x \to a} f(x) = L and lim⁡x→ag(x)=M\lim_{x \to a} g(x) = M both exist, then the limit of a sum, difference, product and constant multiple is the corresponding combination of LL and MM, the limit of a quotient is L/ML/M provided M≠0M \neq 0, and lim⁡f(x)n=Ln\lim f(x)^n = L^n. If ff is continuous at MM then lim⁡f(g(x))=f(M)\lim f(g(x)) = f(M).

The squeeze theorem

If g(x)≤f(x)≤h(x)g(x) \le f(x) \le h(x) near aa (except possibly at aa) and lim⁡x→ag(x)=lim⁡x→ah(x)=L\lim_{x\to a} g(x) = \lim_{x\to a} h(x) = L, then lim⁡x→af(x)=L\lim_{x \to a} f(x) = L.

Because −1≤sin⁡(1/x)≤1-1 \le \sin(1/x) \le 1, multiplying by x2x^2 gives −x2≤x2sin⁡(1/x)≤x2-x^2 \le x^2 \sin(1/x) \le x^2, and both bounds tend to 00, so lim⁡x→0x2sin⁡(1/x)=0\lim_{x \to 0} x^2\sin(1/x) = 0. The same function with xx in place of x2x^2 is squeezed in the same way, but sin⁡(1/x)\sin(1/x) alone has no limit at 00 because it oscillates between −1-1 and 11 infinitely often.

Standard limits

With xx in radians,

lim⁡x→0sin⁡xx=1,lim⁡x→01−cos⁡xx2=12,lim⁡x→0ex−1x=1,lim⁡x→0ln⁡(1+x)x=1, \lim_{x\to 0}\frac{\sin x}{x} = 1, \qquad \lim_{x \to 0}\frac{1 - \cos x}{x^2} = \frac12, \qquad \lim_{x \to 0}\frac{e^x - 1}{x} = 1, \qquad \lim_{x \to 0}\frac{\ln(1+x)}{x} = 1,
lim⁡n→∞(1+1n)n=e,lim⁡x→∞(1+ax)x=ea. \lim_{n \to \infty}\left(1 + \frac{1}{n}\right)^n = e, \qquad \lim_{x \to \infty}\left(1 + \frac{a}{x}\right)^x = e^a.

Exponentials beat powers and powers beat logarithms: for any k>0k > 0, xk/ex→0x^k / e^x \to 0 and (ln⁡x)/xk→0(\ln x)/x^k \to 0 as x→∞x \to \infty.

Indeterminate forms and L'Hôpital's rule

The forms 00\frac{0}{0}, ∞∞\frac{\infty}{\infty}, 0⋅∞0 \cdot \infty, ∞−∞\infty - \infty, 1∞1^\infty, 000^0 and ∞0\infty^0 do not determine a limit by themselves. L'Hôpital's rule handles the first two: if ff and gg are differentiable near aa, lim⁡f=lim⁡g=0\lim f = \lim g = 0 (or both tend to ±∞\pm\infty), and lim⁡f′(x)g′(x)\lim \frac{f'(x)}{g'(x)} exists or is infinite, 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)}.

It can be applied repeatedly. For example

lim⁡x→0ex−1−xx2=lim⁡x→0ex−12x=lim⁡x→0ex2=12. \lim_{x \to 0}\frac{e^x - 1 - x}{x^2} = \lim_{x \to 0}\frac{e^x - 1}{2x} = \lim_{x \to 0}\frac{e^x}{2} = \frac12.

The other forms are first rewritten as a quotient. For 0⋅∞0\cdot\infty, write xln⁡x=ln⁡x1/xx \ln x = \frac{\ln x}{1/x} as x→0+x \to 0^+; this is of the form ∞/∞\infty/\infty, and the rule gives 1/x−1/x2=−x→0\frac{1/x}{-1/x^2} = -x \to 0. For the forms 1∞1^\infty, 000^0 and ∞0\infty^0, take logarithms: if y=f(x)g(x)y = f(x)^{g(x)} then ln⁡y=g(x)ln⁡f(x)\ln y = g(x)\ln f(x), find the limit of that, and exponentiate. Thus for y=xxy = x^x as x→0+x \to 0^+, ln⁡y=xln⁡x→0\ln y = x\ln x \to 0, so y→e0=1y \to e^0 = 1.

Continuity

A function ff is continuous at aa if f(a)f(a) is defined, lim⁡x→af(x)\lim_{x \to a} f(x) exists, and the two are equal. It is continuous on an interval if it is continuous at every point there (at an endpoint, using the one-sided limit). Polynomials, exe^x, sin⁡x\sin x and cos⁡x\cos x are continuous everywhere, rational functions are continuous wherever the denominator is non-zero, and sums, products, quotients (with non-zero denominator) and compositions of continuous functions are continuous.

There are three ways for continuity to fail at aa.

KindWhat happensExample at x=0x = 0
Removablethe limit exists but differs from f(a)f(a) or f(a)f(a) is undefinedsin⁡xx\dfrac{\sin x}{x}
Jumpboth one-sided limits exist but are different∣x∣x\dfrac{\vert x\vert}{x}
Infinite or oscillatinga one-sided limit is infinite or does not exist1x\dfrac1x, sin⁡1x\sin\dfrac1x

A removable discontinuity is repaired by redefining f(a)f(a) as the limit.

Theorems for continuous functions on a closed interval

Let ff be continuous on [a,b][a, b].

  • The intermediate value theorem: ff takes every value between f(a)f(a) and f(b)f(b) at some point of [a,b][a,b]. In particular, if f(a)f(a) and f(b)f(b) have opposite signs, ff has a zero in (a,b)(a, b).
  • The extreme value theorem: ff attains a maximum and a minimum on [a,b][a,b]. Both hypotheses are needed: f(x)=1/xf(x) = 1/x on (0,1](0, 1] has no maximum, and f(x)=xf(x) = x on (0,1)(0,1) has no maximum or minimum.
  • ff is bounded on [a,b][a, b], and is in fact uniformly continuous there.

As an example of the intermediate value theorem, f(x)=x3+x−1f(x) = x^3 + x - 1 has f(0)=−1<0f(0) = -1 < 0 and f(1)=1>0f(1) = 1 > 0, so it has a root in (0,1)(0, 1). A continuous map from [0,1][0,1] to itself has a fixed point, since g(x)=f(x)−xg(x) = f(x) - x satisfies g(0)≥0g(0) \ge 0 and g(1)≤0g(1) \le 0.

Continuity and differentiability

A function differentiable at aa is continuous at aa, because f(a+h)−f(a)=h⋅f(a+h)−f(a)h→0⋅f′(a)=0f(a + h) - f(a) = h \cdot \frac{f(a+h) - f(a)}{h} \to 0 \cdot f'(a) = 0. The converse fails: ∣x∣|x| is continuous at 00 but has a corner there, with one-sided gradients −1-1 and 11.

Limits of sequences

A sequence an→La_n \to L if ∣an−L∣|a_n - L| eventually stays below any given positive number. A monotonic bounded sequence converges. If ff is continuous and an+1=f(an)a_{n+1} = f(a_n) with an→La_n \to L, then L=f(L)L = f(L). For a1=1a_1 = 1, an+1=2+ana_{n+1} = \sqrt{2 + a_n}, the terms increase and are bounded above by 22 (if an<2a_n < 2 then an+1<4=2a_{n+1} < \sqrt 4 = 2), so they converge to a limit satisfying L=2+LL = \sqrt{2 + L}, that is L2−L−2=0L^2 - L - 2 = 0, and since L>0L > 0, L=2L = 2.

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