condition n equation 条件方程
oseen n equation 奥新方程
motion n equation 运动方程
Poisson n equation 泊松方程
boltzmann n equation 麦克斯韦
pulsation n equation 脉动方程
The integral N-S equation is regarded as a special diffusion equation and the pressure term, convective term are regarded as source terms.
将此N S方程看作一个特殊的扩散方程,将压力项与对流项看作是源项,得到一个积分方程。
The equation is impossible for any value of n greater than 2.
这个等式对于任何大于2的数值都不成立。
The other element of the equation, b, turns out to be directly related to T1. It is calculated from the relationship between the logarithms of the attack number, n, and the attack interval, Tn.
至于这个公式里的其他元素,b和T1直接相关,它由袭击次数n的对数和袭击间隔Tn的关系计算得出。
And we talked about the equation you can use for radial nodes last time, and that's just n minus 1 minus l.
我们讲过这个用于,计算径向节点的方程,也就是n减去l减去1
So, what we have left in our equation is only one part that n we haven't explained yet, and that is that n value.
现在方程里只剩下一个常数,我们还没有解释,这就是。
So it's a more specific version of the equation where we have the n final equal to 2.
当我们令n等于2时,使这个这个方程变成更具体的版本。
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