Step 1: Recognize vector field.
\[
F = -y \hat{i} + x \hat{j}
\]
This corresponds to a rotational field (like circulation around origin).
Step 2: Line integral.
By Green's theorem:
\[
\oint F \cdot dl = \iint \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) dA
\]
where \(F = P\hat{i} + Q\hat{j}\).
Here: \(P = -y, \; Q = x\).
\[
\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = \frac{\partial (x)}{\partial x} - \frac{\partial (-y)}{\partial y} = 1 - (-1) = 2
\]
Step 3: Area of region.
Region is cardioid: \(r = 1 + \cos\theta\).
Area:
\[
A = \frac{1}{2} \int_{0}^{2\pi} r^2 d\theta = \frac{1}{2} \int_{0}^{2\pi} (1 + \cos\theta)^2 d\theta
\]
\[
= \frac{1}{2} \int_{0}^{2\pi} (1 + 2\cos\theta + \cos^2\theta) d\theta
\]
\[
= \frac{1}{2} \left[ \int_0^{2\pi} 1 d\theta + 2\int_0^{2\pi}\cos\theta d\theta + \int_0^{2\pi}\frac{1+\cos2\theta}{2} d\theta \right]
\]
\[
= \frac{1}{2} \left[ 2\pi + 0 + \pi \right] = \frac{3\pi}{2}
\]
Step 4: Integral value.
\[
\oint F \cdot dl = 2 \times A = 2 \times \frac{3\pi}{2} = 3\pi \approx 9.42
\]
Final Answer:
\[
\boxed{9.42}
\]
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