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To find the value of the divergence theorem for the given vector field ( mathbf{D} = 2xy mathbf{i} + x^2 mathbf{j} ), over the rectangular parallelepiped bounded by (x = 0) and (1), (y = 0) and (2), (z = 0) and (3), we first need to understand and apply the divergence theorem itself. The divergence theorem relates the flow (flux) of a vector field through a closed surface to the divergence of the field in the volume enclosed by the surface. Mathematically, it is represented as:
[ intintint_V (nabla cdot mathbf{D}) dV = intint_S mathbf{D} cdot mathbf{n} dS ]
Where:
– (V) is the volume inside the surface (S),
– (mathbf{D}) is the vector field,
– (nabla cdot mathbf{D}) represents the divergence of (mathbf{D}),
– (dV) is a volume element, and
– (dS) is an element of the surface area with (mathbf{n}) being the outward facing normal.
Given the vector field (mathbf{D} = 2xy mathbf{i} + x^2 mathbf
b
Explanation: While evaluating surface integral, there has to be two variables and one
constant compulsorily. ∫∫D.ds = ∫∫Dx=0 dy dz + ∫∫Dx=1 dy dz + ∫∫Dy=0 dx dz + ∫∫Dy=2 dx
dz + ∫∫Dz=0 dy dx + ∫∫Dz=3 dy dx. Put D in equation, the integral value we get is 12.