To determine the number of local maximum and minimum points for the function \( f(x) = \int_0^{x^2} \frac{t^2 - 8t + 15}{e^t} dt \), we need to analyze its derivative. Using the Leibniz rule for differentiation under the integral sign, we have:
\[ f'(x) = \frac{d}{dx}\left(\int_0^{x^2} \frac{t^2 - 8t + 15}{e^t} dt\right) = \frac{d}{dx}\left(x^2\right) \cdot \frac{x^2 - 8x + 15}{e^{x^2}} = 2x \cdot \frac{x^2 - 8x + 15}{e^{x^2}} \]
Setting \( f'(x) = 0 \), we solve:
\[ 2x(x^2 - 8x + 15) = 0 \]This gives:\
We then perform a sign test to identify intervals of increase and decrease. Consider points before 0, between 0 and 3, 3 and 5, and after 5 in the expression \( x(x-3)(x-5) \). Substituting a test value from each interval, we determine:
Local extrema occur at changes from increasing to decreasing (local maximum) or from decreasing to increasing (local minimum). Hence, we find:
As both local maxima and minima occur twice considering points beyond 5, the respective counts of local maximum and minimum points are: 2 and 2.
We have $$f(x)=\int_{0}^{x^{2}} e^{t}(t^{2}-8t+15)\,dt.$$ Differentiating, $$f'(x)=2x\,e^{x^{2}}(x^{2}-3)(x^{2}-5).$$ So the critical points are $$x=0,\quad x=\pm\sqrt{3},\quad x=\pm\sqrt{5}.$$
The sign changes of \(f'\) (or the monotonicity chart) give:
The only disputed point is \(x=0\). We can test it with the second derivative. Write \(f'(x)=2x\,g(x)\) where \(g(x)=e^{x^{2}}(x^{2}-3)(x^{2}-5)\). Then $$f''(x)=2g(x)+2x g'(x).$$ In particular at \(x=0\), $$f''(0)=2g(0)=2\cdot e^{0}(0-3)(0-5)=2\cdot(-3)\cdot(-5)=30>0.$$ Since \(f''(0)>0\), \(x=0\) is a local minimum.
Therefore the function has:
Conclusion: number of local maxima = 2, number of local minima = 2.
If $y = 5 \cos x - 3 \sin x$, prove that $\frac{d^2y}{dx^2} + y = 0$.
Show that \( f(x) = \tan^{-1}(\sin x + \cos x) \) is an increasing function in \( \left[ 0, \frac{\pi}{4} \right] \).
A small point of mass \(m\) is placed at a distance \(2R\) from the center \(O\) of a big uniform solid sphere of mass \(M\) and radius \(R\). The gravitational force on \(m\) due to \(M\) is \(F_1\). A spherical part of radius \(R/3\) is removed from the big sphere as shown in the figure, and the gravitational force on \(m\) due to the remaining part of \(M\) is found to be \(F_2\). The value of the ratio \( F_1 : F_2 \) is: 
A transparent block A having refractive index $ \mu_2 = 1.25 $ is surrounded by another medium of refractive index $ \mu_1 = 1.0 $ as shown in figure. A light ray is incident on the flat face of the block with incident angle $ \theta $ as shown in figure. What is the maximum value of $ \theta $ for which light suffers total internal reflection at the top surface of the block ?