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. \[ \boxed{{Correct options: (B), (D)}} \]
If \( \vec{u}, \vec{v}, \vec{w} \) are non-coplanar vectors and \( p, q \) are real numbers, then the equality:
\[ [3\vec{u} \quad p\vec{v} \quad p\vec{w}] - [p\vec{v} \quad \vec{w} \quad q\vec{u}] - [2\vec{w} \quad q\vec{v} \quad q\vec{u}] = 0 \]
holds for:
In the Wheatstone bridge shown below, the sensitivity of the bridge in terms of change in balancing voltage \( E \) for unit change in the resistance \( R \), in V/Ω, is __________ (round off to two decimal places).
The relationship between two variables \( x \) and \( y \) is given by \( x + py + q = 0 \) and is shown in the figure. Find the values of \( p \) and \( q \). Note: The figure shown is representative.