The magnetic field at point A is given by \( B_A = \mu₀I/(2r_A) \). The magnetic field at point B, considering two turns, is \( B_B = \mu₀I/r_B \). Given a constant wire length, \( 2\pi r_A = 4\pi r_B \), which implies \( r_B = r_A/2 \). Consequently, the ratio \( B_A/B_B \) is \( 1/4 \).