Consider:
\[ g(f(x)) = \begin{cases} g(\log_e x), & x > 0 \\ g(e^{-x}), & x \leq 0 \end{cases} \]
For \(x > 0\), we have:
\[ f(x) = \log_e x \implies g(f(x)) = g(\log_e x) = \log_e x \quad (\text{since } \log_e x \geq 0) \]
For \(x \leq 0\), we have:
\[ f(x) = e^{-x} \implies g(f(x)) = g(e^{-x}) = e^{-x} \quad (\text{since } e^{-x} > 0 \text{ for all } x \leq 0) \]
Thus, the function \(g(f(x))\) is given by:
\[ g(f(x)) = \begin{cases} \log_e x, & x > 0 \\ e^{-x}, & x \leq 0 \end{cases} \]
Analyzing this function, we observe:
For \(x > 0\), \(g(f(x)) = \log_e x\) is an increasing function but not onto as it maps to \((0, \infty)\).
For \(x \leq 0\), \(g(f(x)) = e^{-x}\) is a decreasing function and does not cover the entire range of real numbers.
Therefore, \(g \circ f\) is neither one-one nor onto.
Determine the properties of the composite function \( g \circ f: \mathbb{R} \to \mathbb{R} \), where \( f \) and \( g \) are piecewise defined.
To analyze \( g \circ f \), we compute \( (g \circ f)(x) = g(f(x)) \) for different ranges of \( x \), using the definitions of \( f \) and \( g \). We then check for continuity and differentiability at the transition points.
Step 1: Write definitions of \( f \) and \( g \).
\[ f(x) = \begin{cases} \ln x, & x > 0, \\ e^{-x}, & x \leq 0, \end{cases} \quad g(x) = \begin{cases} x, & x \geq 0, \\ e^x, & x < 0. \end{cases} \]
Step 2: Compute \( g(f(x)) \) for \( x > 0 \).
For \( x > 0 \), \( f(x) = \ln x \).
We need \( g(\ln x) \), which depends on whether \( \ln x \geq 0 \) or \( \ln x < 0 \).
So for \( x > 0 \): \[ (g \circ f)(x) = \begin{cases} x, & 0 < x < 1, \\ \ln x, & x \geq 1. \end{cases} \]
Step 3: Compute \( g(f(x)) \) for \( x \leq 0 \).
For \( x \leq 0 \), \( f(x) = e^{-x} \).
Since \( x \leq 0 \), \( -x \geq 0 \), so \( e^{-x} \geq 1 > 0 \). Thus \( f(x) > 0 \) for \( x \leq 0 \).
Since \( f(x) > 0 \), we use \( g(y) = y \) for \( y \geq 0 \).
So \( g(f(x)) = f(x) = e^{-x} \) for \( x \leq 0 \).
Step 4: Write complete definition of \( g \circ f \).
\[ (g \circ f)(x) = \begin{cases} e^{-x}, & x \leq 0, \\ x, & 0 < x < 1, \\ \ln x, & x \geq 1. \end{cases} \]
Step 5: Check continuity at \( x = 0 \).
Left-hand limit as \( x \to 0^- \): \( \lim_{x \to 0^-} e^{-x} = e^0 = 1 \).
Right-hand limit as \( x \to 0^+ \): \( \lim_{x \to 0^+} x = 0 \).
Since \( 1 \neq 0 \), \( g \circ f \) is discontinuous at \( x = 0 \).
Step 6: Check continuity at \( x = 1 \).
Left-hand limit as \( x \to 1^- \): \( \lim_{x \to 1^-} x = 1 \).
Right-hand limit as \( x \to 1^+ \): \( \lim_{x \to 1^+} \ln x = \ln 1 = 0 \).
Since \( 1 \neq 0 \), \( g \circ f \) is discontinuous at \( x = 1 \).
Step 7: Check differentiability.
Since the function is discontinuous at \( x = 0 \) and \( x = 1 \), it is not differentiable at these points.
On intervals \( (-\infty, 0) \), \( (0, 1) \), \( (1, \infty) \), the function is differentiable (as composition of differentiable functions).
Step 8: Conclusion.
The function \( g \circ f \) is discontinuous at \( x = 0 \) and \( x = 1 \), hence not one-one, not onto, and not differentiable at these points.
From the definition: For \( x \leq 0 \), \( (g \circ f)(x) = e^{-x} \in [1, \infty) \); for \( 0 < x < 1 \), \( (g \circ f)(x) = x \in (0, 1) \); for \( x \geq 1 \), \( (g \circ f)(x) = \ln x \in [0, \infty) \). So range is \( (0, 1) \cup [1, \infty) = (0, \infty) \), not all \( \mathbb{R} \), so not onto.
Also, not one-one since multiple \( x \) give same value (e.g., \( x = -1 \) gives \( e^1 \), \( x = e^e \) gives \( \ln(e^e) = e \), etc.).
Therefore, \( g \circ f \) is neither one-one nor onto.
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,