dfrac ({mu )_(0)I}(pi R)(dfrac (1)(2)+dfrac (pi )(6))-|||-dfrac ({mu )_(0)I}(pi
(B) (mu ,dfrac (1)(sqrt {2pi )})-|||-(C) (mu ,dfrac (1)(2)), (D)(0,σ).
dfrac ({U)_(0)I}(2R)-|||-D . dfrac ({U)_(0)I}(2pi R)
在真空中有一根半径为R的半圆形细导线,流过的电流为I,则圆心处的磁感应强度为-|||-(A) dfrac ({mu )_(0)}(4pi )dfrac (I)(
=dfrac (Q)(4pi {varepsilon )_(0)r}-|||-(D) =dfrac (Q)(4pi {varepsilon )_(0)(r)^2
(D) =dfrac ({mu )_(0)(I)_(1)(I)_(2)}(2pi )ln dfrac (b)(a)-|||-Ai-|||-I1-|||-C I2
C-|||-R-|||-+Q-|||-(B) dfrac (qQ)(4pi {varepsilon )_(0)R} , -dfrac (qQ)(4pi {var
内分布,电流为I,规定垂直纸面向里为正,-|||-则在点O的磁感强度为 ()-|||-R-|||-O-|||----|||-A .dfrac ({mu )_(0
(B) dfrac (lambda )(2pi {varepsilon )_(0)a}. (C) dfrac (lambda )(4pi {varepsilon
._(M)-(U)_(N)= -dfrac ({mu )_(0)lg g}(2pi )tln dfrac (a+l)(a) ___ o