Evaluate the limit: lim⁡x→∞tan⁡(5x1/3)log⁡e(1+3x2)(tan⁡−1(3x))2(e5x4/3−1)\lim_{x \to \infty} \frac{\tan\left(5x^{1/3}\right) \log_e(1 + 3x^2)}{\left(\tan^{-1}(3\sqrt{x})\right)^2 \left(e^{5x^{4/3}} - 1\right)} is equal to:

Answer: The limit does not exist.

Step-by-step solution

Step 1: Simplify terms using standard limits

When evaluating limits as x→∞x \to \infty, we often use standard limit approximations. For very large xx, we can simplify terms like tan⁡−1(3x)\tan^{-1}(3\sqrt{x}) and e5x4/3−1e^{5x^{4/3}} - 1.

Step 2: Approximate terms for large x

As x→∞x \to \infty, 3x→∞3\sqrt{x} \to \infty, so tan⁡−1(3x)\tan^{-1}(3\sqrt{x}) approaches π2\frac{\pi}{2}. Also, e5x4/3e^{5x^{4/3}} becomes much larger than 1, so e5x4/3−1≈e5x4/3e^{5x^{4/3}} - 1 \approx e^{5x^{4/3}}. For log⁡e(1+3x2)\log_e(1 + 3x^2), as x→∞x \to \infty, 3x23x^2 dominates 1, so log⁡e(1+3x2)≈log⁡e(3x2)\log_e(1 + 3x^2) \approx \log_e(3x^2).

Step 3: Substitute approximations into the limit expression

Now we substitute these approximations back into the original limit expression. The denominator simplifies to (π2)2e5x4/3(\frac{\pi}{2})^2 e^{5x^{4/3}}.

Step 4: Analyze the behavior of the terms

As x→∞x \to \infty, 5x1/3→∞5x^{1/3} \to \infty. The tangent function tan⁡(y)\tan(y) oscillates between −∞-\infty and ∞\infty as y→∞y \to \infty. It does not approach a single finite value.

Step 5: Determine the limit

The numerator contains an oscillating term tan⁡(5x1/3)\tan(5x^{1/3}) and a term (log⁡e(3)+2log⁡e(x))(\log_e(3) + 2\log_e(x)) that goes to ∞\infty. The denominator e5x4/3e^{5x^{4/3}} goes to ∞\infty much faster than the numerator. However, due to the oscillating nature of the tangent function, the limit does not exist.

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