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The identity for \( \nabla \cdot (\phi\mathbf{A}) \) with \( \phi \) scalar is

  • A.\( \mathbf{A} \cdot \nabla\phi \) alone
  • B.\( \phi\,\nabla \cdot \mathbf{A} + \mathbf{A} \cdot \nabla\phi \)
  • C.\( \phi\,\nabla \cdot \mathbf{A} \) alone
  • D.\( \phi\,\nabla \cdot \mathbf{A} - \mathbf{A} \cdot \nabla\phi \)

Answer: B

The operator differentiates both factors, and the term acting on the scalar has to be contracted with the vector to stay a scalar:

\[ \nabla \cdot (\phi\mathbf{A}) \;=\; \phi\,(\nabla \cdot \mathbf{A}) + \mathbf{A} \cdot \nabla\phi. \]

The sign is positive, as in an ordinary product rule; the minus sign belongs to no standard identity of this kind

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