To evaluate the given limit, we first express it mathematically:
\(\lim_{{x \to \infty}} \frac{{(2x^2 - 3x + 5) \left( 3x - 1 \right)^{x/2}}}{{(3x^2 + 5x + 4) \sqrt{(3x + 2)^x}}}.\)
The expression involves exponential terms, and it is beneficial to factor out the highest powers of \(x\) from both the numerator and the denominator. Let's perform the simplification step-by-step:
Substitute these back into the original limit:
\(\lim_{{x \to \infty}} \frac{{2x^2 \cdot 3^{x/2} \cdot x^{x/2}}}{{3x^2 \cdot 3^{x/2} \cdot x^{x/2}}}.\)
Canceling out the common terms \(3^{x/2} \cdot x^{x/2}\) from both the numerator and the denominator, we simplify the expression to:
\(\lim_{{x \to \infty}} \frac{2}{3}.\)
Therefore, the value of the limit is:
\(\frac{2}{3\sqrt{e}}\) (option D).
If \( \lim_{x \to 0} \left( \frac{\tan x}{x} \right)^{\frac{1}{x^2}} = p \), then \( 96 \ln p \) is: 32
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,