Question:medium

If \(\vec{A} = \vec{\nabla} \times \vec{F}\), then \(\oiint_S \vec{A} \cdot \hat{n} dS\) (for any closed surface S) is:

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The identity \(\text{div}(\text{curl} \, \vec{F}) = 0\) is extremely useful. It implies that a vector field which is the curl of another field (like the magnetic field \(\vec{B} = \vec{\nabla} \times \vec{A}\)) must be solenoidal (divergence-free). This means it has no sources or sinks, and its field lines must form closed loops.
Updated On: Feb 10, 2026
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The Correct Option is A

Solution and Explanation

Step 1: Apply the Divergence Theorem (Gauss's Theorem). The Divergence Theorem connects a surface integral over a closed surface S to a volume integral over the enclosed volume V: \[ \oiint_S \vec{A} \cdot \hat{n} dS = \iiint_V (\vec{abla} \cdot \vec{A}) dV \]
Step 2: Substitute the given expression for \(\vec{A}\). Given \(\vec{A} = \vec{abla} \times \vec{F}\), substitute this into the volume integral: \[ \iiint_V \vec{abla} \cdot (\vec{abla} \times \vec{F}) dV \]
Step 3: Use the vector calculus identity for the divergence of a curl. A key vector calculus identity states that the divergence of the curl of any vector field is identically zero: \[ \vec{abla} \cdot (\vec{abla} \times \vec{F}) = 0 \]
Step 4: Evaluate the integral. As the integrand is zero, the volume integral evaluates to zero: \[ \iiint_V (0) dV = 0 \] Consequently, the surface integral is also zero.
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