In spherical coordinates, for a vector field \( \mathbf{f}(R) = \mathbf{a}_R F(R) \), the divergence is: \[ \nabla \cdot \mathbf{f} = \frac{1}{R^2} \frac{d}{dR} \left( R^2 F(R) \right) \] Given \( F(R) = \frac{1}{R^n} \), we get: \[ \nabla \cdot \mathbf{f} = \frac{1}{R^2} \frac{d}{dR} \left( R^2 \cdot \frac{1}{R^n} \right) = \frac{1}{R^2} \cdot \frac{d}{dR} \left( R^{2-n} \right) = \frac{1}{R^2} \cdot (2 - n) R^{1 - n} = (2 - n) R^{-1 - n} \] For the divergence to be independent of \( R \), the exponent of \( R \) must be zero: \[ -1 - n = 0 \Rightarrow n = -1 \] Now test if there are other such values. Let’s try the expression: \[ \nabla \cdot \mathbf{f} = (2 - n) R^{-1 - n} \] This will be independent of \( R \) if the exponent is zero: \[ -1 - n = 0 \Rightarrow n = -1 \] So, only \( n = -1 \) strictly satisfies divergence being constant. However, if we want zero divergence, then: \[ \nabla \cdot \mathbf{f} = 0 \Rightarrow (2 - n) R^{-1 - n} = 0 \Rightarrow 2 - n = 0 \Rightarrow n = 2 \] So, for: - \( n = -1 \): divergence is constant (independent of \( R \)) - \( n = 2 \): divergence is zero, which is also independent of \( R \)
Hence, both \( n = -1 \) and \( n = 2 \) are correct. \[ \boxed{{Correct options: (B), (D)}} \]
a times b is equal to
Given an open-loop transfer function \(GH = \frac{100}{s}(s+100)\) for a unity feedback system with a unit step input \(r(t)=u(t)\), determine the rise time \(t_r\).
Consider a linear time-invariant system represented by the state-space equation: \[ \dot{x} = \begin{bmatrix} a & b -a & 0 \end{bmatrix} x + \begin{bmatrix} 1 0 \end{bmatrix} u \] The closed-loop poles of the system are located at \(-2 \pm j3\). The value of the parameter \(b\) is: