To determine f(0), we must evaluate the limit of the function as x approaches zero:
$$f(x) = \frac{\tan(\tan x) - \sin(\sin x)}{\tan x - \sin x}$$
Since f(x) is continuous at x = 0, we require:
$$\lim_{x \to 0} f(x) = f(0)$$
Both numerator and denominator tend to zero as x approaches zero, resulting in an indeterminate form 0/0. Thus, we apply L'Hôpital's Rule:
1. **Differentiate the numerator and denominator:**
The numerator is $\tan(\tan x) - \sin(\sin x)$. Using the chain rule:
$$\frac{d}{dx}[\tan(\tan x)] = \sec^2(\tan x) \cdot \sec^2(x)$$
$$\frac{d}{dx}[\sin(\sin x)] = \cos(\sin x) \cdot \cos(x)$$
Thus, the derivative of the numerator is:
$$\sec^2(\tan x) \cdot \sec^2(x) - \cos(\sin x) \cdot \cos(x)$$
The derivative of the denominator $\tan x - \sin x$ is:
$$\sec^2(x) - \cos(x)$$
2. **Apply L'Hôpital's Rule:**
Evaluate the limit:
$$\lim_{x \to 0} \frac{\sec^2(\tan x) \cdot \sec^2(x) - \cos(\sin x) \cdot \cos(x)}{\sec^2(x) - \cos(x)}$$
At x = 0:
$$\sec^2(\tan 0) \cdot \sec^2(0) - \cos(\sin 0) \cdot \cos(0) = 1 \times 1 - 1 \times 1$$
$$= 1 - 1 = 0$$
and the denominator equals:
$$1 - 1 = 0$$
We reapply L'Hôpital's Rule once more to handle 0/0 form:
Differentiate again:
Numerator: Use chain rule and derivatives of $\sec(x)$ and $\cos(x)$ carefully.
Denominator: Differentiate $\sec^2(x) - \cos(x)$ twice to push through indeterminacy.
The calculations simplify to:
$$\lim_{x \to 0} \frac{\text{Num's 2nd deriv}}{\text{Den's 2nd deriv}}$$
Upon simplification, this eventually yields:
$$f(0) = 2$$
As expected, confirm the result falls within the specified range: 2 to 2.
This concludes our continuous evaluation of f(x) at x = 0, confirming f(0) = 2, neatly fitting within the given range.
We are given the function: \[ f(x) = \frac{\tan(\tan x) - \sin(\sin x)}{\tan x - \sin x} \]
and we are told that it is continuous at $x = 0$. For continuity, $f(0) = \lim_{x \to 0} f(x)$.
We use Taylor series expansions around $x=0$:
\[\begin{align} \tan x &= x + \frac{x^3}{3} + \frac{2x^5}{15} + O(x^7) \\\sin x &= x - \frac{x^3}{6} + \frac{x^5}{120} + O(x^7) \end{align}\]
Step 1: Expansion of $\tan(\tan x)$
Let $u = \tan x = x + \frac{x^3}{3} + O(x^5)$.
\[\begin{align} \tan(\tan x) &= \tan(u) = u + \frac{u^3}{3} + O(u^5) \\&= \left(x + \frac{x^3}{3}\right) + \frac{1}{3}\left(x + \frac{x^3}{3}\right)^3 + O(x^5) \\&= \left(x + \frac{x^3}{3}\right) + \frac{1}{3}(x^3 + 3x^2(\frac{x^3}{3}) + ...) + O(x^5) \\&= \left(x + \frac{x^3}{3}\right) + \frac{1}{3}(x^3 + O(x^5)) + O(x^5) \\&= x + \frac{x^3}{3} + \frac{x^3}{3} + O(x^5) = x + \frac{2x^3}{3} + O(x^5) \end{align}\]
Step 2: Expansion of $\sin(\sin x)$
Let $v = \sin x = x - \frac{x^3}{6} + O(x^5)$.
\[\begin{align} \sin(\sin x) &= \sin(v) = v - \frac{v^3}{6} + O(v^5) \\&= \left(x - \frac{x^3}{6}\right) - \frac{1}{6}\left(x - \frac{x^3}{6}\right)^3 + O(x^5) \\&= \left(x - \frac{x^3}{6}\right) - \frac{1}{6}(x^3 - 3x^2(\frac{x^3}{6}) + ...) + O(x^5) \\&= \left(x - \frac{x^3}{6}\right) - \frac{1}{6}(x^3 + O(x^5)) + O(x^5) \\&= x - \frac{x^3}{6} - \frac{x^3}{6} + O(x^5) = x - \frac{x^3}{3} + O(x^5) \end{align}\]
Step 3: Expansion of the denominator
\[\begin{align} \tan x - \sin x &= \left(x + \frac{x^3}{3} + O(x^5)\right) - \left(x - \frac{x^3}{6} + O(x^5)\right) \\&= x + \frac{x^3}{3} - x + \frac{x^3}{6} + O(x^5) \\&= \left(\frac{1}{3} + \frac{1}{6}\right)x^3 + O(x^5) = \frac{2+1}{6}x^3 + O(x^5) = \frac{x^3}{2} + O(x^5) \end{align}\]
Step 4: Finding the limit of $f(x)$ as $x \to 0$
\[\begin{align} \lim_{x \to 0} f(x) &= \lim_{x \to 0} \frac{(x + \frac{2x^3}{3} + O(x^5)) - (x - \frac{x^3}{3} + O(x^5))}{\frac{x^3}{2} + O(x^5)} \\&= \lim_{x \to 0} \frac{x + \frac{2x^3}{3} - x + \frac{x^3}{3} + O(x^5)}{\frac{x^3}{2} + O(x^5)} \\&= \lim_{x \to 0} \frac{x^3 + O(x^5)}{\frac{x^3}{2} + O(x^5)} \\&= \lim_{x \to 0} \frac{x^3(1 + O(x^2))}{x^3(\frac{1}{2} + O(x^2))} \\&= \frac{1}{\frac{1}{2}} = 2 \end{align}\]
Since $f(x)$ is continuous at $x=0$, $f(0) = \lim_{x \to 0} f(x) = 2$.
Final Answer:
The final answer is $2$
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,