Sequence Convergence & Limits - Calculus 2

  1. Consider the sequence an=(−1)n(n2−1)n2+n+1a_n = \frac{(-1)^n (n^2 - 1)}{n^2 + n + 1}. Which of the following is true?
    Answer: The sequence diverges. For an alternating sequence to converge, the limit of the absolute value of its terms must be 0. Let's examine lim⁡n→∞∣an∣=lim⁡n→∞n2−1n2+n+1\lim_{n \to \infty} |a_n| = \lim_{n \to \infty} \frac{n^2 - 1}{n^2 + n + 1}. Since the degrees of the numerator and denominator are equal, the limit is the ratio of the leading coefficients, which is 1/1=11/1 = 1. Because lim⁡n→∞∣an∣=1≠0\lim_{n \to \infty} |a_n| = 1 \neq 0, the sequence does not converge. The terms for even nn approach 1, while the terms for odd nn approach -1. The sequence oscillates between values close to 1 and -1 and therefore diverges.
  2. What is the limit of the sequence defined by an=n1/(n+1)a_n = n^{1/(n+1)}?
    Answer: 1 This limit is of the indeterminate form ∞0\infty^0. Let L=lim⁡n→∞n1/(n+1)L = \lim_{n \to \infty} n^{1/(n+1)}. We can find the limit of its natural logarithm: ln⁡(L)=lim⁡n→∞ln⁡(n1/(n+1))=lim⁡n→∞ln⁡(n)n+1\ln(L) = \lim_{n \to \infty} \ln(n^{1/(n+1)}) = \lim_{n \to \infty} \frac{\ln(n)}{n+1}. This is an ∞/∞\infty/\infty indeterminate form, so we can use L'Hôpital's rule. Taking the derivative of the numerator and denominator with respect to nn gives lim⁡n→∞1/n1=0\lim_{n \to \infty} \frac{1/n}{1} = 0. Since ln⁡(L)=0\ln(L) = 0, we have L=e0=1L = e^0 = 1.
  3. Find the limit of the sequence an=nsin⁡(πn)a_n = n \sin(\frac{\pi}{n}).
    Answer: π\pi This limit is of the indeterminate form ∞⋅0\infty \cdot 0. We can rewrite it as an=sin⁡(π/n)1/na_n = \frac{\sin(\pi/n)}{1/n}. This is now in the 0/00/0 form, suitable for L'Hôpital's rule. Let's consider the function f(x)=sin⁡(π/x)1/xf(x) = \frac{\sin(\pi/x)}{1/x}. Taking derivatives of the numerator and denominator with respect to xx gives: lim⁡x→∞cos⁡(π/x)⋅(−π/x2)−1/x2=lim⁡x→∞πcos⁡(π/x)\lim_{x \to \infty} \frac{\cos(\pi/x) \cdot (-\pi/x^2)}{-1/x^2} = \lim_{x \to \infty} \pi \cos(\pi/x). As x→∞x \to \infty, π/x→0\pi/x \to 0, and cos⁡(π/x)→cos⁡(0)=1\cos(\pi/x) \to \cos(0) = 1. Thus, the limit is π\pi. This is a variation of the fundamental trigonometric limit lim⁡θ→0sin⁡(θ)θ=1\lim_{\theta \to 0} \frac{\sin(\theta)}{\theta} = 1.
  4. The sequence {an}\{a_n\} is defined such that a2k=k+1ka_{2k} = \frac{k+1}{k} for even indices and a2k−1=4k−54k−3a_{2k-1} = \frac{4k-5}{4k-3} for odd indices. What can be concluded about the sequence {an}\{a_n\}?
    Answer: The sequence converges to 1. A sequence converges if and only if all of its subsequences converge to the same limit. Here, the sequence is partitioned into even and odd terms. We find the limit of each subsequence. For the even terms: lim⁡k→∞a2k=lim⁡k→∞k+1k=1\lim_{k \to \infty} a_{2k} = \lim_{k \to \infty} \frac{k+1}{k} = 1. For the odd terms: lim⁡k→∞a2k−1=lim⁡k→∞4k−54k−3=44=1\lim_{k \to \infty} a_{2k-1} = \lim_{k \to \infty} \frac{4k-5}{4k-3} = \frac{4}{4} = 1. Since both the subsequence of even terms and the subsequence of odd terms converge to the same limit, 1, the entire sequence {an}\{a_n\} converges to 1.
  5. Evaluate the limit lim⁡n→∞3n+1+n4n!+3n\lim_{n \to \infty} \frac{3^{n+1} + n^4}{n! + 3^n}.
    Answer: 0 To evaluate this limit, we compare the rates of growth of the terms. In the numerator, the exponential term 3n+13^{n+1} grows much faster than the polynomial term n4n^4. In the denominator, the factorial term n!n! grows much faster than the exponential term 3n3^n. Therefore, the limit is determined by the ratio of the fastest-growing terms: lim⁡n→∞3n+1n!\lim_{n \to \infty} \frac{3^{n+1}}{n!}. It is a standard result that factorials grow faster than any exponential function, so lim⁡n→∞cnn!=0\lim_{n \to \infty} \frac{c^n}{n!} = 0 for any constant cc. Thus, the limit is 0.
  6. The sequence {an}\{a_n\} converges to LL. According to the formal definition of a limit, this means that for any ϵ>0\epsilon > 0, there exists an integer NN such that for all n>Nn > N, which of the following inequalities holds?
    Answer: ∣an−L∣<ϵ|a_n - L| < \epsilon The formal definition of the limit of a sequence states that a sequence {an}\{a_n\} converges to a limit LL if for every positive number ϵ\epsilon, there is an integer NN such that for all n>Nn > N, the distance between ana_n and LL is less than ϵ\epsilon. This is expressed mathematically as ∣an−L∣<ϵ|a_n - L| < \epsilon. The other options confuse the roles of the limit LL, the index NN, and the error tolerance ϵ\epsilon.
  7. A sequence {gn}\{g_n\} satisfies 0<gn≤1n0 < g_n \leq \frac{1}{n} for all n≥1n \geq 1, and ∑n=1∞gn\sum_{n=1}^{\infty} g_n converges. If hn=g1+g2+⋯+gnnh_n = \frac{g_1 + g_2 + \cdots + g_n}{n}, what can be concluded about lim⁡n→∞hn\lim_{n \to \infty} h_n?
    Answer: lim⁡n→∞hn=0\lim_{n \to \infty} h_n = 0 by Stolz-Cesàro theorem applied to the ratio of partial sums to nn Since ∑n=1∞gn\sum_{n=1}^{\infty} g_n converges, we have lim⁡n→∞gn=0\lim_{n \to \infty} g_n = 0. Let Sn=g1+g2+⋯+gnS_n = g_1 + g_2 + \cdots + g_n. Then hn=Snnh_n = \frac{S_n}{n}. Since {Sn}\{S_n\} converges to ∑n=1∞gn\sum_{n=1}^{\infty} g_n, by Stolz-Cesàro theorem: lim⁡n→∞Snn=lim⁡n→∞Sn+1−Sn(n+1)−n=lim⁡n→∞gn+1=0\lim_{n \to \infty} \frac{S_n}{n} = \lim_{n \to \infty} \frac{S_{n+1} - S_n}{(n+1) - n} = \lim_{n \to \infty} g_{n+1} = 0. Choice A mentions Cesàro mean theorem incorrectly. Choice B is wrong because convergent series do guarantee this limit exists and equals 0. Choice D confuses the sum of the series with the limit of averages.
  8. Let an=∫nn+1sin⁡(x)xdxa_n = \int_n^{n+1} \frac{\sin(x)}{x} dx. Find lim⁡n→∞an\lim_{n \to \infty} a_n.
    Answer: 0 We can use the Squeeze Theorem. For xx in the interval [n,n+1][n, n+1] where n≥1n \ge 1, we know −1≤sin⁡(x)≤1-1 \le \sin(x) \le 1 and 1n+1≤1x≤1n\frac{1}{n+1} \le \frac{1}{x} \le \frac{1}{n}. This gives the bounds −1n≤sin⁡(x)x≤1n\frac{-1}{n} \le \frac{\sin(x)}{x} \le \frac{1}{n}. Integrating this inequality over the interval [n,n+1][n, n+1] of length 1, we get ∫nn+1−1ndx≤an≤∫nn+11ndx\int_n^{n+1} \frac{-1}{n} dx \le a_n \le \int_n^{n+1} \frac{1}{n} dx, which simplifies to −1n≤an≤1n\frac{-1}{n} \le a_n \le \frac{1}{n}. As n→∞n \to \infty, both −1n\frac{-1}{n} and 1n\frac{1}{n} approach 0. By the Squeeze Theorem, lim⁡n→∞an=0\lim_{n \to \infty} a_n = 0.
  9. A student wants to find the limit of an=n+cos⁡(n)na_n = \frac{n + \cos(n)}{n}. They argue that since this is an ∞/∞\infty/\infty form, they can use L'Hôpital's rule on f(x)=x+cos⁡(x)xf(x) = \frac{x+\cos(x)}{x}. The derivative of the numerator is 1−sin⁡(x)1-\sin(x) and the derivative of the denominator is 1. Since lim⁡x→∞(1−sin⁡(x))\lim_{x \to \infty} (1-\sin(x)) does not exist, they conclude the original sequence diverges. What is wrong with this reasoning?
    Answer: The original expression can be simplified algebraically, and L'Hôpital's rule is unnecessary. The student's conclusion that the sequence diverges is incorrect. The best approach is to simplify the expression algebraically: an=nn+cos⁡(n)n=1+cos⁡(n)na_n = \frac{n}{n} + \frac{\cos(n)}{n} = 1 + \frac{\cos(n)}{n}. We can then use the Squeeze Theorem on the cos⁡(n)n\frac{\cos(n)}{n} term. Since −1≤cos⁡(n)≤1-1 \le \cos(n) \le 1, we have −1n≤cos⁡(n)n≤1n\frac{-1}{n} \le \frac{\cos(n)}{n} \le \frac{1}{n}. As n→∞n \to \infty, this term is squeezed to 0. Thus, lim⁡n→∞an=1+0=1\lim_{n \to \infty} a_n = 1+0=1. The student's reasoning is flawed because L'Hôpital's rule being inconclusive (when the limit of derivatives DNE) does not imply the original limit diverges. The fundamental error was choosing a complicated and ultimately inconclusive method instead of a simple algebraic one.
  10. Find the limit of the sequence defined by an=ln⁡(n2+en)na_n = \frac{\ln(n^2 + e^n)}{n}.
    Answer: 1 To find the limit, we can consider the corresponding function f(x)=ln⁡(x2+ex)xf(x) = \frac{\ln(x^2 + e^x)}{x} and apply L'Hôpital's rule, as the limit is of the indeterminate form ∞/∞\infty/\infty. The derivative of the numerator is 2x+exx2+ex\frac{2x + e^x}{x^2 + e^x} and the derivative of the denominator is 1. The new limit is lim⁡x→∞2x+exx2+ex\lim_{x \to \infty} \frac{2x + e^x}{x^2 + e^x}. This is still ∞/∞\infty/\infty. We can divide the numerator and denominator by the fastest-growing term, exe^x, to get lim⁡x→∞2x/ex+1x2/ex+1\lim_{x \to \infty} \frac{2x/e^x + 1}{x^2/e^x + 1}. Since lim⁡x→∞xp/ex=0\lim_{x \to \infty} x^p/e^x = 0 for any power p, the limit simplifies to 0+10+1=1\frac{0+1}{0+1} = 1.
  11. Find the limit of the sequence an=(n2+n−n)(−1)na_n = (\sqrt{n^2+n} - n)(-1)^n.
    Answer: The sequence diverges. This is an alternating sequence. We first examine the limit of its magnitude, ∣an∣=n2+n−n|a_n| = \sqrt{n^2+n} - n. This is an ∞−∞\infty - \infty indeterminate form. We multiply by the conjugate: ∣an∣=(n2+n−n)(n2+n+n)n2+n+n=nn2+n+n|a_n| = \frac{(\sqrt{n^2+n}-n)(\sqrt{n^2+n}+n)}{\sqrt{n^2+n}+n} = \frac{n}{\sqrt{n^2+n}+n}. Taking the limit, we get lim⁡n→∞nn2+n+n=lim⁡n→∞11+1/n+1=11+1=12\lim_{n \to \infty} \frac{n}{\sqrt{n^2+n}+n} = \lim_{n \to \infty} \frac{1}{\sqrt{1+1/n}+1} = \frac{1}{1+1} = \frac{1}{2}. Since lim⁡n→∞∣an∣=1/2≠0\lim_{n \to \infty} |a_n| = 1/2 \neq 0, the sequence {an}\{a_n\} does not converge to 0. The terms oscillate between values approaching 1/2 and -1/2, so the sequence diverges.
  12. Which of the following statements about a sequence {an}\{a_n\} of real numbers is always true?
    Answer: If the sequence {an}\{a_n\} is not bounded, then it diverges. A convergent sequence must be bounded. The contrapositive of this statement is that if a sequence is not bounded, it must diverge. This is always true. Choice A is false; the harmonic series an=1/na_n = 1/n provides a counterexample. Choice B is false; the sequence an=(−1)na_n = (-1)^n is bounded but diverges. Choice D is false; the sequence an=na_n = n is monotonic but diverges.
  13. Find the limit of the sequence an=n(n2+4−n)a_n = n(\sqrt{n^2+4} - n).
    Answer: 2 The expression is of the indeterminate form ∞⋅(∞−∞)\infty \cdot (\infty - \infty). To resolve this, we multiply the term in the parenthesis by its conjugate: n2+4−n=(n2+4−n)(n2+4+n)n2+4+n=(n2+4)−n2n2+4+n=4n2+4+n\sqrt{n^2+4} - n = \frac{(\sqrt{n^2+4} - n)(\sqrt{n^2+4} + n)}{\sqrt{n^2+4} + n} = \frac{(n^2+4)-n^2}{\sqrt{n^2+4} + n} = \frac{4}{\sqrt{n^2+4} + n}. Substituting back, an=n⋅4n2+4+n=4nn2+4+na_n = n \cdot \frac{4}{\sqrt{n^2+4} + n} = \frac{4n}{\sqrt{n^2+4} + n}. Now, we can find the limit by dividing the numerator and denominator by nn: lim⁡n→∞4n2+4n+1=lim⁡n→∞41+4/n2+1=41+0+1=42=2\lim_{n \to \infty} \frac{4}{\frac{\sqrt{n^2+4}}{n} + 1} = \lim_{n \to \infty} \frac{4}{\sqrt{1+4/n^2} + 1} = \frac{4}{\sqrt{1+0} + 1} = \frac{4}{2} = 2.
  14. Find the limit of the sequence an=∑k=1n1n+ka_n = \sum_{k=1}^n \frac{1}{n+k}.
    Answer: ln⁡(2)\ln(2) This sequence can be interpreted as a Riemann sum. We can factor out 1/n1/n from the sum: an=∑k=1n1n(1+k/n)=1n∑k=1n11+k/na_n = \sum_{k=1}^n \frac{1}{n(1+k/n)} = \frac{1}{n} \sum_{k=1}^n \frac{1}{1+k/n}. This is the right Riemann sum for the function f(x)=11+xf(x) = \frac{1}{1+x} on the interval [0,1][0, 1] with Δx=1/n\Delta x = 1/n. As n→∞n \to \infty, this sum converges to the definite integral: ∫0111+xdx=[ln⁡∣1+x∣]01=ln⁡(2)−ln⁡(1)=ln⁡(2)\int_0^1 \frac{1}{1+x} dx = [\ln|1+x|]_0^1 = \ln(2) - \ln(1) = \ln(2).
  15. Find the limit of the sequence an=5n+(−2)n5n−(−2)na_n = \frac{5^n + (-2)^n}{5^n - (-2)^n}.
    Answer: 1 The dominant term in both the numerator and the denominator is 5n5^n, as it grows much faster than (−2)n(-2)^n. To find the limit, we can divide both the numerator and the denominator by this dominant term: an=1+(−2/5)n1−(−2/5)na_n = \frac{1 + (-2/5)^n}{1 - (-2/5)^n}. As n→∞n \to \infty, the term (−2/5)n(-2/5)^n approaches 0 because its base has an absolute value less than 1. Therefore, the limit is lim⁡n→∞an=1+01−0=1\lim_{n \to \infty} a_n = \frac{1+0}{1-0} = 1.
  16. The sequence {an}\{a_n\} is defined by a1=1a_1=1 and an+1=6+ana_{n+1} = \sqrt{6+a_n}. It can be shown that the sequence is increasing and bounded above by 3. What is the limit of the sequence?
    Answer: 3 The problem states that the sequence is increasing and bounded above, so by the Monotonic Sequence Theorem, it converges to a limit LL. We can find LL by taking the limit of the recurrence relation: lim⁡n→∞an+1=lim⁡n→∞6+an\lim_{n \to \infty} a_{n+1} = \lim_{n \to \infty} \sqrt{6+a_n}, which gives L=6+LL = \sqrt{6+L}. Squaring both sides yields L2=6+LL^2 = 6+L, or L2−L−6=0L^2 - L - 6 = 0. This factors as (L−3)(L+2)=0(L-3)(L+2) = 0, so the possible limits are L=3L=3 and L=−2L=-2. Since a1=1a_1=1 is positive and the square root function always produces a non-negative result, all terms of the sequence are positive. Thus, the limit must be positive, so L=3L=3.
  17. Find the limit of the sequence an=1nln⁡(n!nn)a_n = \frac{1}{n} \ln\left(\frac{n!}{n^n}\right).
    Answer: -1 We can use the properties of logarithms to rewrite the expression: an=1n(ln⁡(n!)−ln⁡(nn))=1n(∑k=1nln⁡(k)−nln⁡(n))=1n∑k=1nln⁡(k)−ln⁡(n)a_n = \frac{1}{n}(\ln(n!) - \ln(n^n)) = \frac{1}{n}(\sum_{k=1}^{n} \ln(k) - n\ln(n)) = \frac{1}{n}\sum_{k=1}^{n} \ln(k) - \ln(n). The term 1n∑k=1nln⁡(k)\frac{1}{n}\sum_{k=1}^{n} \ln(k) can be seen as an approximation of the integral 1n∫1nln⁡(x)dx\frac{1}{n}\int_1^n \ln(x) dx. Evaluating the integral gives 1n[xln⁡(x)−x]1n=1n(nln⁡(n)−n+1)=ln⁡(n)−1+1n\frac{1}{n}[x\ln(x) - x]_1^n = \frac{1}{n}(n\ln(n) - n + 1) = \ln(n) - 1 + \frac{1}{n}. Substituting this back gives an≈(ln⁡(n)−1+1n)−ln⁡(n)=−1+1na_n \approx (\ln(n) - 1 + \frac{1}{n}) - \ln(n) = -1 + \frac{1}{n}. As n→∞n \to \infty, this approaches -1. A more formal approach uses Stirling's approximation for ln⁡(n!)\ln(n!), which also yields the limit -1.
  18. A sequence is defined by a1=1a_1 = 1 and an+1=3an+2an+2a_{n+1} = \frac{3a_n + 2}{a_n + 2}. If the sequence converges, what is its limit?
    Answer: 2 Let the limit of the sequence be LL. Taking the limit of both sides of the recurrence relation gives L=3L+2L+2L = \frac{3L + 2}{L + 2}. We solve this equation for LL: L(L+2)=3L+2  ⟹  L2+2L=3L+2  ⟹  L2−L−2=0L(L+2) = 3L+2 \implies L^2 + 2L = 3L+2 \implies L^2 - L - 2 = 0. This factors into (L−2)(L+1)=0(L-2)(L+1) = 0, giving possible limits of L=2L=2 and L=−1L=-1. Since a1=1a_1=1 is positive, and the recurrence relation will produce a positive an+1a_{n+1} if ana_n is positive, all terms of the sequence are positive. Therefore, the limit must be L=2L=2.
  19. What is the limit of the sequence an=(n−1n+1)na_n = \left(\frac{n-1}{n+1}\right)^n?
    Answer: e−2e^{-2} This limit is of the indeterminate form 1∞1^\infty. We can rewrite the base as n−1n+1=n+1−2n+1=1−2n+1=1+−2n+1\frac{n-1}{n+1} = \frac{n+1-2}{n+1} = 1 - \frac{2}{n+1} = 1 + \frac{-2}{n+1}. The expression becomes an=(1+−2n+1)na_n = \left(1 + \frac{-2}{n+1}\right)^n. This resembles the standard limit form lim⁡m→∞(1+x/m)m=ex\lim_{m \to \infty} (1 + x/m)^m = e^x. We can rewrite our expression as an=(1+−2n+1)n+1−1=(1+−2n+1)n+1⋅(1+−2n+1)−1a_n = \left(1 + \frac{-2}{n+1}\right)^{n+1-1} = \left(1 + \frac{-2}{n+1}\right)^{n+1} \cdot \left(1 + \frac{-2}{n+1}\right)^{-1}. As n→∞n \to \infty, the first term approaches e−2e^{-2} and the second term approaches 1−1=11^{-1}=1. Thus, the limit is e−2e^{-2}.
  20. Consider the sequence bn=ln⁡(n3+n2)ln⁡(n4+2n3+1)b_n = \frac{\ln(n^3 + n^2)}{\ln(n^4 + 2n^3 + 1)}. To find lim⁡n→∞bn\lim_{n \to \infty} b_n, which approach correctly identifies the limit?
    Answer: Rewrite as 3ln⁡(n)+ln⁡(1+1/n)4ln⁡(n)+ln⁡(1+2/n+1/n4)\frac{3\ln(n) + \ln(1 + 1/n)}{4\ln(n) + \ln(1 + 2/n + 1/n^4)} which approaches 34\frac{3}{4} Using logarithm properties: bn=ln⁡(n3)+ln⁡(1+1/n)ln⁡(n4)+ln⁡(1+2/n+1/n4)=3ln⁡(n)+ln⁡(1+1/n)4ln⁡(n)+ln⁡(1+2/n+1/n4)b_n = \frac{\ln(n^3) + \ln(1 + 1/n)}{\ln(n^4) + \ln(1 + 2/n + 1/n^4)} = \frac{3\ln(n) + \ln(1 + 1/n)}{4\ln(n) + \ln(1 + 2/n + 1/n^4)}. As n→∞n \to \infty, ln⁡(1+1/n)→0\ln(1 + 1/n) \to 0 and ln⁡(1+2/n+1/n4)→0\ln(1 + 2/n + 1/n^4) \to 0, so the limit becomes 3ln⁡(n)4ln⁡(n)=34\frac{3\ln(n)}{4\ln(n)} = \frac{3}{4}. Choice A is incorrect because you can't factor constants out of logarithms that way. Choice B applies L'Hôpital's rule incorrectly. Choice D ignores the different powers in the logarithmic arguments.

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