The gravitational potential \( V \) is related to the gravitational field \( E \) by: \[ E = -\frac{dV}{dx} \] We are given that \( E = \frac{K}{x^3} \), and we need to find \( V \).
Integrating \( E \) with respect to \( x \), we get: \[ V = -\int E \, dx = -\int \frac{K}{x^3} \, dx = \frac{K}{2x^2} \] Thus, the gravitational potential at distance \( x \) is \( \frac{K}{2x^2} \).
Final Answer: \( \frac{K}{2x^2} \)