Step 1: The function \( f(x) = |x^2 - 1| \) is defined as the absolute value of \( x^2 - 1 \). To analyze the function, we consider two cases for \( x^2 - 1 \):
\[ f(x) = \begin{cases} x^2 - 1 & \text{if } x^2 \geq 1, \\ 1 - x^2 & \text{if } x^2 < 1. \end{cases} \]
This piecewise function describes a parabola that is reflected along the x-axis when \( |x| < 1 \) and a parabola opening upwards for \( |x| \geq 1 \).
Step 2: Local minima occur where the function reaches its lowest value. First, notice that \( f(x) = 0 \) when \( x = \pm 1 \) because:
\[ f(x) = |x^2 - 1| = 0 \quad \text{when } x^2 - 1 = 0 \quad \implies \quad x = \pm 1. \]
At \( x = 1 \) and \( x = -1 \), the function transitions from decreasing to increasing, indicating that these are points of local minima.
Step 3: Local maxima occur where the function reaches its highest value within a given interval. Notice that the function reaches a local maximum at \( x = 0 \), because:
\[ f(0) = |0^2 - 1| = | -1| = 1. \]
The function \( f(x) \) decreases on the interval \( (-1, 1) \) and then increases after \( x = \pm 1 \), so \( x = 0 \) is a local maximum.
Step 4: Therefore, the function \( f(x) \) has local minima at \( x = \pm 1 \) and a local maximum at \( x = 0 \).
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).