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冷却塔二维轴对称坐标N-S方程推导详细过程:连续性方程:mrrxxSrvvrvvtX方向动量方程:XrxxxrxxxFxvrvrrrvxvrxrxpvvrrrvvrxrvt1322111对于理想不可压缩气体:0v对于定常流:0xvt,0t,不考虑原项Sm=0所以连续性方程:0rvrvvvrrxxX方向动量方程:XrxxxrxxFxvrvrrrvxvrxrxpvvrrrvvrxr1322111XrxxxrxxFxvrvrrrxvrxrxpvvrrrvvrxr12111XrxxxrxxFxvrvrrrxvrxrxpvvrrrvvrxr1211XrxxxxrxxFxvrvrrrrxxvrxvxrrxpvvrrrvvrxr12211XrxrxxxxrxxFrrxvrvrxvrvrrxxvrxvxpvvrrrvvrxr1221122XrxrxxxxrxxFrrxvrvrxvrrvrxxvrxvxpvvrrrvvrxr122112222rvxrvxvxxvrxvrrxrx22XrrxxxxxrxxFrvxrrxvrvrrvrxxvrxvxpvvrrrvvrxr12112222XrrxxxxxrxxFrvxrrxvrvrrvrxxvrxpxvvvrrrvvrxr12112222rvrrrrrrvrrvxxx1122XrrxxxxrxxFrvxrrxvrrxxvrrvrrrxpxvvvrrrvvrxr1211122XrrxxxxrxxFrvxrrxvrrxxvrxprvrrrxvvvrrrvvrxr1211122rxvxvrrrrrxvrrrr211XrrrxxxxrxxFrvxrxvxvrrrrxxvrxprvrrrxvvvrrrvvrxr22212111rvxxvrvxvxrvxrxvrxrxrr222XrxrxrxxxrxxFrvxrxxvrrvxxvxvrrrxprvrrrxvrxrvvrrrvvrxr11111122XrrxrxxxrxxFrxrvrvrxvxvrrrxprvrrrxvrxrvvrrrvvrxr11111122因为:0xrrx所以:XxrxxxrxxFxvxvrrrxprvrrrxvrxrvvrrrvvrxr2211111XxrxxxrxxFxvxvrrrxprvrrrxvrxrvvrrrvvx221111
本文标题:冷却塔二维轴对称N-S方程详细推导
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