Swapping the limits of integration in a one-dimensional integral results in the negation of the integral, expressed as ∫_a^b f(x) dx = -∫_b^a f(x) dx. This principle is generally accepted, but there are instances where it may be presented as a special case without clarification. In electromagnetism, the potential is defined using the negative of the integral with swapped limits, raising questions about the necessity of this approach. The discussion suggests that this convention may stem from the common practice of defining potential from a point at infinity to a local point. Understanding these nuances is essential for clarity in mathematical applications.