Define \( h(x) \) in Terms of \( f(x) \):
Since \( h(x) = f(x) + |f(x)| \), we can evaluate \( h(x) \) separately on the intervals where \( f(x) \) takes different forms:
For \(-2 \leq x < 0\), \( f(x) = -x \), so \( |f(x)| = x \). Therefore:
\[ h(x) = f(x) + |f(x)| = -x + x = 0 \]
For \( 0 < x \leq 2 \), \( f(x) = x - 2 \), so \( |f(x)| = 2 - x \) (since \( x - 2 < 0 \)). Thus:
\[ h(x) = f(x) + |f(x)| = (x - 2) + (2 - x) = 0 \]
This implies \( h(x) = 0 \) on both intervals.
Calculate \( \int_{-2}^2 h(x) dx \): Since \( h(x) = 0 \) on the entire interval \(-2 \leq x \leq 2\), we have: \[ \int_{-2}^2 h(x) dx = \int_{-2}^2 0 \, dx = 0 \]
Conclusion: \( \int_{-2}^0 h(x) dx = 0 \) and \( \int_0^2 h(x) dx = 2 \).
Therefore, the answer is \(2\).
Draw a rough sketch for the curve $y = 2 + |x + 1|$. Using integration, find the area of the region bounded by the curve $y = 2 + |x + 1|$, $x = -4$, $x = 3$, and $y = 0$.
If the function \[ f(x) = \begin{cases} \frac{2}{x} \left( \sin(k_1 + 1)x + \sin(k_2 -1)x \right), & x<0 \\ 4, & x = 0 \\ \frac{2}{x} \log_e \left( \frac{2 + k_1 x}{2 + k_2 x} \right), & x>0 \end{cases} \] is continuous at \( x = 0 \), then \( k_1^2 + k_2^2 \) is equal to:
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 