Given:
Step 1: Rewrite the equation using trigonometric identity: \[ p \cos \theta + q \sin \theta = \sqrt{p^2 + q^2} \cos(\theta - \alpha) \] where \( \alpha \) is an angle such that \( \cos \alpha = \frac{p}{\sqrt{p^2 + q^2}} \) and \( \sin \alpha = \frac{q}{\sqrt{p^2 + q^2}} \).
Step 2: Analyze the range of the left side: \[ -\sqrt{p^2 + q^2} \leq p \cos \theta + q \sin \theta \leq \sqrt{p^2 + q^2} \]
Step 3: Compare with the given condition \( |r| > \sqrt{p^2 + q^2} \):
Conclusion: The equation \( p \cos \theta + q \sin \theta = r \) has no real solution under the given condition.
The correct answer is (D) no real solution.
The given equation is:
\[ p\cos\theta + q\sin\theta = r \]
We can rewrite this equation using the auxiliary angle method. Let \( p = R\cos\phi \) and \( q = R\sin\phi \), where \( R = \sqrt{p^2 + q^2} \) and \( \phi = \arctan(q/p) \).
Then the equation becomes:
\[ R\cos\phi\cos\theta + R\sin\phi\sin\theta = r \] \[ R\cos(\theta - \phi) = r \] \[ \cos(\theta - \phi) = \frac{r}{R} = \frac{r}{\sqrt{p^2 + q^2}} \]
Since \( |r| > \sqrt{p^2 + q^2} \), we have \( \left|\frac{r}{R}\right| > 1 \).
However, the range of the cosine function is \([-1, 1]\).
Therefore, there are no real solutions for \( \theta \) in this case.
The equation has no solution.
Kepler's second law (law of areas) of planetary motion leads to law of conservation of