We are tasked with evaluating the integral: \[ \int_{-\pi/2}^{\pi/2} \sin^9 x \cos^2 x \, dx \] First, observe that the integrand consists of powers of sine and cosine.
We can use the identity \( \cos^2 x = \frac{1 + \cos(2x)}{2} \) to simplify the integral: \[ \int_{-\pi/2}^{\pi/2} \sin^9 x \cos^2 x \, dx = \int_{-\pi/2}^{\pi/2} \sin^9 x \left( \frac{1 + \cos(2x)}{2} \right) \, dx \]
Now, split the integral: \[ = \frac{1}{2} \int_{-\pi/2}^{\pi/2} \sin^9 x \, dx + \frac{1}{2} \int_{-\pi/2}^{\pi/2} \sin^9 x \cos(2x) \, dx \] The first integral is an odd function \( \sin^9 x \), and when integrated over symmetric limits from \( -\pi/2 \) to \( \pi/2 \), it evaluates to 0.
The second integral involves \( \sin^9 x \cos(2x) \), which is also an odd function, so it too evaluates to 0.
Therefore, the total integral evaluates to 0.
Kepler's second law (law of areas) of planetary motion leads to law of conservation of