Step 1: Use vector calculus identities.
There are two fundamental vector identities that can solve this problem without direct calculation:
1. The curl of the gradient of any scalar field is always zero: \(\vec{\nabla} \times (\vec{\nabla}\phi) = \vec{0}\).
2. The divergence of the gradient is the Laplacian: \(\vec{\nabla} \cdot (\vec{\nabla}\phi) = \nabla^2\phi\).
Step 2: Apply the identities to the given problem.
- Curl of \(\vec{A}\): We are given \(\vec{A} = \vec{\nabla}\phi\). Using the first identity, we immediately know that \(\vec{\nabla} \times \vec{A} = \vec{\nabla} \times (\vec{\nabla}\phi) = \vec{0}\). Therefore, statement C is true and D is false. A vector field that is the gradient of a scalar potential is called a conservative or irrotational field.
- Divergence of \(\vec{A}\): Using the second identity, we need to calculate the Laplacian of \(\phi\).
\[ \vec{\nabla} \cdot \vec{A} = \nabla^2\phi = \frac{\partial^2\phi}{\partial x^2} + \frac{\partial^2\phi}{\partial y^2} + \frac{\partial^2\phi}{\partial z^2} \]
First derivatives are: \(\frac{\partial\phi}{\partial x} = y+z\), \(\frac{\partial\phi}{\partial y} = x+z\), \(\frac{\partial\phi}{\partial z} = y+x\).
Second derivatives are:
\[ \frac{\partial^2\phi}{\partial x^2} = 0, \quad \frac{\partial^2\phi}{\partial y^2} = 0, \quad \frac{\partial^2\phi}{\partial z^2} = 0 \]
Therefore, \(\vec{\nabla} \cdot \vec{A} = 0+0+0=0\). Statement A is true and B is false.
Step 3: Conclude the correct statements.
Both statements A and C are true.