Consider a vector field →A(→r). The closed loop line integral ∮→A.d→l can be expressed as
A
∯(∇×→A).→ds over the closed surface bounded by the loop
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B
∯(∇×→A)dv over the closed volume bounded by the loop
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C
∭(∇.→A)dv over the open volume bounded by the loop
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D
∬(∇×→A).→ds over the open surface bounded by the loop
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Solution
The correct option is D∬(∇×→A).→ds over the open surface bounded by the loop By stoke's theorem ∮→A.d→l=∬(∇×→A).d→S
(i.e closed loop line integral to open surface integral)