curl F ⃗ = ∣ i ⃗ j ⃗ k ⃗ ∂ ∂ x ∂ ∂ y ∂ ∂ z x 2 x y 0 ∣ = y k ⃗ , \text{curl }\vec F=\begin{vmatrix}
\vec i& \vec j & \vec k\\
\frac{\partial}{\partial x}& \frac{\partial}{\partial y}&\frac{\partial}{\partial z}\\
x^2 & xy& 0
\end{vmatrix}=y\vec k, curl F = ∣ ∣ i ∂ x ∂ x 2 j ∂ y ∂ x y k ∂ z ∂ 0 ∣ ∣ = y k ,
curl F ⃗ ⋅ n ⃗ = y , \text{curl}\vec F\cdot \vec n=y, curl F ⋅ n = y ,
∬ S curl F ⃗ ⋅ n ⃗ d S = ∫ 0 1 ∫ 0 1 y d y d x + ∫ 0 1 ∫ − 1 0 y d y d x = ∫ 0 1 y 2 2 ∣ 0 1 d x + ∫ 0 1 y 2 2 ∣ − 1 0 d x = ∫ 0 1 1 2 d x + ∫ 0 1 ( − 1 2 ) d x = 0. \underset{S}{\iint }\text{curl}\vec F\cdot \vec ndS =\int_0^1\int_0^1ydydx+\int_0^1\int_{-1}^0ydydx=\int_0^1\frac{y^2}2|_0^1dx+\int_0^1\frac{y^2}2|_{-1}^0dx=\int_0^1\frac 12dx+\int_0^1(-\frac 12)dx=0. S ∬ curl F ⋅ n d S = ∫ 0 1 ∫ 0 1 y d y d x + ∫ 0 1 ∫ − 1 0 y d y d x = ∫ 0 1 2 y 2 ∣ 0 1 d x + ∫ 0 1 2 y 2 ∣ − 1 0 d x = ∫ 0 1 2 1 d x + ∫ 0 1 ( − 2 1 ) d x = 0.
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