To find \( f(g(x)) \), we first evaluate \( g(x) \) based on the value of \( x \).
\[ g(x) = \begin{cases} e^x, & x \geq 0 \\ x + 1, & x \leq 0 \end{cases} \]
The function \( f \) is defined as \( f(x) = |x - 1| \). Therefore, we have: \[ f(g(x)) = |g(x) - 1|. \]
Case 1: When \( x \geq 0 \)
\[ f(g(x)) = |e^x - 1|. \]
Case 2: When \( x \leq 0 \)
\[ f(g(x)) = |x + 1 - 1| = |x| = -x \quad \text{(since \( x \leq 0 \))}. \]
Analysis of \( f(g(x)) \) - For \( x \geq 0 \), \( f(g(x)) = |e^x - 1| \) is neither one-one nor onto because it cannot cover all values in the codomain (as it is non-negative). For \( x \leq 0 \), \( f(g(x)) = -x \) is also neither one-one nor onto due to its behavior as a non-injective transformation on the interval.
Therefore, the function \( f(g(x)) \) is neither one-one nor onto.
If the domain of the function \( f(x) = \dfrac{1}{\sqrt{10 + 3x - x^2}} + \dfrac{1}{\sqrt{x + |x|}} \) is \( (a, b) \), then \((1 + a)^2 + b^2\) is equal to:
For the AC circuit shown in the figure, $ R = 100 \, \text{k}\Omega $ and $ C = 100 \, \text{pF} $, and the phase difference between $ V_{\text{in}} $ and $ (V_B - V_A) $ is 90°. The input signal frequency is $ 10^x $ rad/sec, where $ x $ is:
Two parabolas have the same focus $(4, 3)$ and their directrices are the $x$-axis and the $y$-axis, respectively. If these parabolas intersect at the points $A$ and $B$, then $(AB)^2$ is equal to:
A point particle of charge \( Q \) is located at \( P \) along the axis of an electric dipole 1 at a distance \( r \) as shown in the figure. The point \( P \) is also on the equatorial plane of a second electric dipole 2 at a distance \( r \). The dipoles are made of opposite charge \( q \) separated by a distance \( 2a \). For the charge particle at \( P \) not to experience any net force, which of the following correctly describes the situation?
