对于空气在竖夹层中自然对流换热,当Gr<2000时( ) A: Nu=1 B: Nu=2 C: Nu=3 D: Nu=4
对于空气在竖夹层中自然对流换热,当Gr<2000时( ) A: Nu=1 B: Nu=2 C: Nu=3 D: Nu=4
下面代码的输出结果是( )。 s=[4,3,6,2] t=sorted(s) print(s) print(t) A: [4, 3, 6, 2] [2, 3, 4, 6] B: [2, 3, 4, 6] [2, 3, 4, 6] C: [4, 3, 6, 2] [4, 3, 6, 2] D: [2, 3, 4, 6] [4, 3, 6, 2]
下面代码的输出结果是( )。 s=[4,3,6,2] t=sorted(s) print(s) print(t) A: [4, 3, 6, 2] [2, 3, 4, 6] B: [2, 3, 4, 6] [2, 3, 4, 6] C: [4, 3, 6, 2] [4, 3, 6, 2] D: [2, 3, 4, 6] [4, 3, 6, 2]
水平角观测某一方向,盘左读数为60°01′06″,盘右读数为240°01′00″,其2C值为(): A: +3″ B: +6″ C: -3″ D: -6″
水平角观测某一方向,盘左读数为60°01′06″,盘右读数为240°01′00″,其2C值为(): A: +3″ B: +6″ C: -3″ D: -6″
中缀表达式3*(4+2*3)-6对应的后缀表达式为( )。 A: 3 4 2 3 * + 6 * - B: 3 4 * 2 3 * + 6 - C: 3 4 2 3 * + * 6 - D: 3 4 + 2 3 * * 6 -
中缀表达式3*(4+2*3)-6对应的后缀表达式为( )。 A: 3 4 2 3 * + 6 * - B: 3 4 * 2 3 * + 6 - C: 3 4 2 3 * + * 6 - D: 3 4 + 2 3 * * 6 -
(接上题)(2)设经分界面反射的波的振幅和入射波的振幅相等,则反射波的波函数是 A: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{2} \right),0\le x\le\dfrac{3\lambda}{4}$ B: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$ C: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{4} \right),0\le x\le\dfrac{3\lambda}{4}$ D: $y_{r}=Acos\left(2\pi \nu t-\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$
(接上题)(2)设经分界面反射的波的振幅和入射波的振幅相等,则反射波的波函数是 A: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{2} \right),0\le x\le\dfrac{3\lambda}{4}$ B: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$ C: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{4} \right),0\le x\le\dfrac{3\lambda}{4}$ D: $y_{r}=Acos\left(2\pi \nu t-\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$
(2)设经分界面反射的波的振幅和入射波的振幅相等,则反射波的波函数是 A: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{2} \right),0\le x\le\dfrac{3\lambda}{4}$ B: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$ C: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{4} \right),0\le x\le\dfrac{3\lambda}{4}$ D: $y_{r}=Acos\left(2\pi \nu t-\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$
(2)设经分界面反射的波的振幅和入射波的振幅相等,则反射波的波函数是 A: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{2} \right),0\le x\le\dfrac{3\lambda}{4}$ B: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$ C: $y_{r}=Acos \left(2\pi \nu t+\dfrac{2\pi\nu}{u}x-\dfrac{\pi}{4} \right),0\le x\le\dfrac{3\lambda}{4}$ D: $y_{r}=Acos\left(2\pi \nu t-\dfrac{2\pi\nu}{u}x \right),0\le x\le\dfrac{3\lambda}{4}$
积分区间为[a, b],Simpson公式的Cotes系数为( ) A: (b-a)/6, 4(b-a)/6, (b-a)/6 B: 1/3, 4/3, 1/3 C: (b-a)/3, 4(b-a)/3, (b-a)/3 D: 1/6 4/6 1/6
积分区间为[a, b],Simpson公式的Cotes系数为( ) A: (b-a)/6, 4(b-a)/6, (b-a)/6 B: 1/3, 4/3, 1/3 C: (b-a)/3, 4(b-a)/3, (b-a)/3 D: 1/6 4/6 1/6
当质点以频率\(\nu\)作简谐振动时,它的动能的变化频率为 A: \(\nu\) B: 2\(\nu\) C: 4\(\nu\) D: \(\nu\)/2
当质点以频率\(\nu\)作简谐振动时,它的动能的变化频率为 A: \(\nu\) B: 2\(\nu\) C: 4\(\nu\) D: \(\nu\)/2
φ(12)=φ(3*4)=φ(2*6)=φ(3)*φ(4)=φ(2)*φ(6
φ(12)=φ(3*4)=φ(2*6)=φ(3)*φ(4)=φ(2)*φ(6
石英、萤石、方解石、正长石的硬度分别是()。 A: 7 4 3 6 B: 6 5 3 7 C: 7 3 6 4 D: 7 6 3 4
石英、萤石、方解石、正长石的硬度分别是()。 A: 7 4 3 6 B: 6 5 3 7 C: 7 3 6 4 D: 7 6 3 4