The Gauss theorem states that the flux "\\oint_{\\partial V} \\left( \\boldsymbol{F} \\cdot \\boldsymbol{n} \\right) dS" of a vector field "\\boldsymbol{F}" over a boundary "\\partial V" of volume "V" is equal to the volume integral "\\int_V \\left( \\nabla \\cdot \\boldsymbol{F} \\right) d V". Calculating the divergence of our vector field, we have "\\nabla \\cdot \\boldsymbol{F} = 3", and the volume integral is
"\\int_V \\left( \\nabla \\cdot \\boldsymbol{F} \\right) d V = 3 \\int_V d V = 3 V = 3 \\pi A^2 H \\, ,"where we have taken into account that "V = \\pi A^2 H".
Answer: "3 \\pi A^2 H".
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