Answer:
U = 1 / r²
Explanation:
In this problem, the task does not require calculating potential energy via the force equation since these two variables are interconnected.
F = - dU / dr
This derivative represents a gradient, meaning it indicates direction, leading us to write
dU = - F. dr
The formula for force becomes
F = B / r³
Now, let’s apply this in the integral:
∫ dU = - ∫ B / r³ dr
Here, the force aligns with the displacement, simplifying the scalar product to the product of magnitudes.
Now, we can solve the integrals:
U - Uo = -B (- / 2r² + 1 / 2r₀²)
To finalize the calculations, a reference point for energy must be designated; commonly, potential energy is set to zero (Uo = 0) at infinity (r = ∞).
U = B / 2r²
Substituting B = 2, we arrive at:
U = 1 / r²