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To compute the divergence of a vector field using the divergence theorem in spherical coordinates, we follow a systematic approach. Given a vector field (mathbf{D} = frac{5r^2}{4} hat{i}) in a coordinate system, we first need to express this field in spherical coordinates and then find its divergence. However, a direct conversion of the given vector field into spherical coordinates poses a challenge since the field is given in a form that suggests it’s already partially in a non-Cartesian form ((frac{5r^2}{4} hat{i}) suggests a dependence on radial distance but uses (hat{i}), which is a Cartesian unit vector). Assuming the intention is to deal with a radially dependent vector field in a spherical context, we can reinterpret the vector field in spherical coordinates, focusing on its radial component only.
Spherical Coordinates Background
In spherical coordinates, a position in space is given by (r) (radial distance), (theta) (polar angle, measured from the positive z-axis), and (phi) (azimuthal angle, measured in the x-y plane from the positive x-axis). Vector fields in spherical coordinates are expressed in terms of these variables and their unit vectors (hat{r}), (hat{theta}), and (hat{phi}).
Given Vector Field
Given the ambiguities in the initial presentation of the vector field, but
c
Explanation: D.ds = ∫∫∫ Div (D) dv, where RHS needs to be computed.
The divergence of D given is, Div(D) = 5r and dv = r2 sin θ dr dθ dφ. On integrating, r =
1->2, φ = 0->2π and θ = 0->π, we get Q = 75 π