To find the domain of the function \(f(x) = \cos^{-1} \left( \frac{2 - |x|}{4} \right) + \left( \log_e (3 - x) \right)^{-1}\), we need to consider the domain restrictions of both parts separately.
Domain of \(\cos^{-1} \left( \frac{2 - |x|}{4} \right)\):
The inverse cosine function, \(\cos^{-1}(y)\), is defined for \(-1 \leq y \leq 1\). Thus, we need:
\(-1 \leq \frac{2 - |x|}{4} \leq 1\)
Solving the inequality:
Domain of \(\left( \log_e(3 - x) \right)^{-1}\):
The natural logarithm, \(\log_e(3-x)\), is defined and positive if \(3 - x > 1\), i.e., \(x < 3\).
But since \(\left(\log_e(3-x)\right)^{-1}\) should be defined, \(\log_e(3-x) \neq 0\).
This implies \(3 - x \neq 1\), hence, \(x \neq 2\).
Combining all conditions:
\(-6 \leq x \leq 6\), \(x < 3\), and \(x \neq 2\).
This means the domain is \([-6, 3) \setminus \{2\}\), which translates to \([-6, 2) \cup (2, 3)\).
Thus, we have:
Therefore, \(\alpha + \beta + \gamma = 6 + 3 + 2 = 11\).
The correct answer is 11.
To find the domain of \( f(x) \), analyze each component individually.
For \( \cos^{-1} \left( \frac{2 - |x|}{4} \right) \) to be defined, \( -1 \leq \frac{2 - |x|}{4} \leq 1 \). Solving these inequalities:
\[ -1 \leq \frac{2 - |x|}{4} \leq 1 \]
leads to \( |x| \leq 6 \), so \( x \in [-6, 6] \).
For \( (\log_e (3 - x))^{-1} \) to be defined, \( \log_e (3 - x) \neq 0 \) and \( 3 - x > 0 \).
Combining these conditions, we have:
\[ x \in [-6, 3) - \{2\} \]
Thus, the domain is \( [-\alpha, \beta) - \{\gamma\} \) where \( \alpha = 6 \), \( \beta = 3 \), and \( \gamma = 2 \).
\( \alpha + \beta + \gamma = 11 \)
The domain of \(y= cos^{-1}|\frac{2-|x|}{4}| log(3 - x)^{-1}\) is [α, β) - {y} then the value of α+β-y =?
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,