To determine the electric field at a point given the electric potential function, we use the concept that the electric field \(\vec{E}\) is the negative gradient of the electric potential \(V\).
The electric potential at any point \((x, y, z)\) is provided as:
\(V = 4xz^2\)
The electric field can be found using the formula:
\(\vec{E} = -\nabla V = -\left(\frac{\partial V}{\partial x}\hat{i} + \frac{\partial V}{\partial y}\hat{j} + \frac{\partial V}{\partial z}\hat{k}\right)\)
Substituting these partial derivatives, the electric field is:
\(\vec{E} = -(4z^2 \hat{i} + 0 \hat{j} + 8xz \hat{k})\)
Now, substitute the given point \((x, y, z) = (1, 0, 2)\) m:
Thus, at the point \((1\text{ m},0,2\text{ m})\), the electric field is \(-16 \hat{i} - 16 \hat{k}\) V/m.
Analyzing the direction, the components of the electric field show that it has a negative \(x\)- and \(z\)-component. Therefore, the electric field is along the negative \()-axis and negative \([z\)-axis.
Hence, the correct answer is "along the negative \(x\)-axis."
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of