已知|overrightarrow(a)•overrightarrow(b)|=3,|overrightarrow(a)×overrightarrow(b)|=
设overrightarrow(a)=(1,-1,2),overrightarrow(b)=(3,-2,-1),则overrightarrow(a)×overr
已知向量overrightarrow(a)=(0,1),overrightarrow(b)=(2,x),若overrightarrow(b)⊥(overrigh
已知overrightarrow(a)=(2,1,-1), overrightarrow(b)=(1,-1,2), 则overrightarrow(a)time
设 overrightarrow(a) = 3, 5, -2,overrightarrow(b) = 2, 1, 4,且已知 lambda overri
overrightarrow(a)=(1,0,1),overrightarrow(b)=(2,1,1),则overrightarrow(a)×overright
已知晶体原胞基矢为:overrightarrow ({a)_(1)}=dfrac (a)(2)overrightarrow (i)+dfrac (sqrt {3
设overrightarrow(a)=(-1,1,2),overrightarrow(b)=(2,-2,-4),则向量|overrightarrow(a)×ov
设单位向量overrightarrow(a),overrightarrow(b)与u轴的夹角分别为(2π)/(3),(π)/(4),则overrightarro
设overrightarrow(a)=(1,1,4),overrightarrow(b)=(1,-2,2),则overrightarrow(a)+overrig