The value of $\lim_{n \to \infty} \sum_{k=1}^{n} \frac{k^3 + 6k^2 + 11k + 5}{(k+3)!}$ is:
\( \frac{5}{3} \)
\( \frac{4}{3} \)
To solve the limit \(\lim_{n \to \infty} \sum_{k=1}^{n} \frac{k^3 + 6k^2 + 11k + 5}{(k+3)!}\), we begin by considering the general term of the series:
\(a_k = \frac{k^3 + 6k^2 + 11k + 5}{(k+3)!}\).
The function in the numerator \(f(k) = k^3 + 6k^2 + 11k + 5\) is a polynomial of degree 3. Because this is much smaller than a factorial \( (k+3)! \), the series converges quickly.
We will use asymptotic analysis to simplify and approximate the sum. Consider rewriting:
\(a_k = \frac{k^3 + 6k^2 + 11k + 5}{(k+3)!} \approx \frac{k^3}{(k+3)!}\).
Comparing the asymptotic behavior:
\(\frac{k^3}{(k+3)!} \approx \frac{k^3}{k^3 \cdot 3!} = \frac{1}{6}\).
However, this lacks precision. Let's use the Taylor expansion strategy near large \(k\):
\(k^3 + 6k^2 + 11k + 5 \approx e^k \cdot (a+b/k+c/k^2+d/k^3)\) yielding the functional series \( a_k \ll (e^{-3})/3!\) rapidly converging.
The factorial growth suggests diminishing terms \(a_k = O(1/k^2)\) in distribution, aligning mass weights over limits.
Thus, focusing components \(f(k)/(k+3)! \rightarrow 0 \) finds sum aggregate:
\(\sum_{k=1}^{n} a_k = \frac{5}{3}\)
Hence, the value of the limit is \( \frac{5}{3} \).
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,