The equation B(x,t)•l - B(x+dx,t)•l in Maxwell's Eqn 34.16 is derived from the convention of line integration around a rectangle in a counter-clockwise direction. This approach aligns with the right-hand rule, where B(x,t) is considered positive and B(x+dx,t) negative due to their respective orientations relative to the integration path. The magnetic field segment B is parallel to the integration direction, while the segment (B + dB) is anti-parallel. This distinction is crucial for correctly applying the principles of electromagnetism. Understanding these conventions is essential for interpreting Maxwell's equations accurately.