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Divergence of [x*y, -y^2/2, 0]
\nabla\cdot\left\langle x y,\ - \frac{y^{2}}{2},\ 0 \right\rangle
Step by step
- \mathbf{F} = \left\langle x y,\ - \frac{y^{2}}{2},\ 0 \right\rangle,\quad \nabla\cdot\mathbf{F} = \frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} + \frac{\partial R}{\partial z}
The divergence adds up how fast each component grows along its own axis.
- \frac{\partial P}{\partial x} = \frac{\partial }{\partial x}\left(x y\right) = y
Differentiate the x-component with respect to x, holding y and z constant.
- \frac{\partial Q}{\partial y} = \frac{\partial }{\partial y}\left(- \frac{y^{2}}{2}\right) = - y
Differentiate the y-component with respect to y, holding x and z constant.
- \frac{\partial R}{\partial z} = \frac{\partial }{\partial z}\left(0\right) = 0
Differentiate the z-component with respect to z, holding x and y constant.
- \nabla\cdot\mathbf{F} = \left(y\right) + \left(- y\right) + \left(0\right) = 0
Add the three partial derivatives.
- \nabla\cdot\mathbf{F} = 0
Zero divergence everywhere: the field has no sources or sinks. For a velocity field this is incompressible flow.
Reveal the answer
\nabla\cdot\mathbf{F} = 0