原油管道生产能耗理论计算过程分析

2025-03-30 02:14:25
推荐回答(1个)
回答(1):

1.热油管路的稳态轴向温降

管道沿程的温度分布可表示为:

油气管道能效管理

式中:G 为原油的质量流量,kg/s;c为平均温度下原油的比热容,J/(kg·℃);D为管道外径,m;L为管道加热输送的长度,m;K为管道的总传热系数,W/(m2·℃);TR为管道起点油温,℃;TL为距起点为L处的油温,℃;T0为周围介质温度,埋地管道则为管中心埋深处的自然地温,℃;i为油流的水力坡降,g为重力加速度。

在推导上式时,假定水力坡降i为定值,实际上热油管道的水力坡降沿程是变化的。水力坡降要由管道的摩阻计算得出,在进行温度分布计算时,它还未精确给出,只能近似取值计算或迭代求解;也可以将管路分段,然后对每一段同步进行水力和热力计算即可。

忽略摩擦热的影响,令b=0,代入上式,得到苏霍夫公式:

油气管道能效管理

2.热能消耗的计算

加热站的有效热负荷:

油气管道能效管理

t小时内,燃料油消耗量:

油气管道能效管理

t小时内,输送1万t原油1km的距离所消耗的燃料:

油气管道能效管理

式中:q为加热炉有效热负荷,kW;G 为油流质量流量,kg/s;c为平均温度下的油品比热容,kJ/(kg·℃);TR为出站温度,℃;Tz为进站温度,℃;So为加热用燃料油消耗量,kg;E为燃料油低位热值,kJ/kg;η为加热系统效率;Sop为燃料油单耗,kg/(104t·km);L为管长,km。

3.热油管道的摩阻计算

列宾宗公式:

油气管道能效管理

其中,

式中:Q为体积流量,m3/s;v为油品运动粘度,m2/s;d为管道内径,m;L为管线长度,km。达西参数A、β、m是随流态变化而变化的,它们的值与各流态区沿程摩阻的计算式如表3-1所示。

表3-1 不同流态时A、m、β值

其中:

油气管道能效管理

式中:e为管面平均绝对当量粗糙度,m;£为管面相对粗糙度,ε=2e/d。水力坡降按下式计算:

油气管道能效管理

4.动力消耗

机械能消耗为克服高差和克服原油输送时的摩阻损失。泵提供给单位质量原油的有效能头(扬程)为:

油气管道能效管理

式中:Zz为管段终点高程,m;ZQ为管段起点处高程,m;hf为沿程摩阻损失,m;hmi为各站站内摩阻,m。

泵的有效功率为

油气管道能效管理

式中:N有效为泵的有效功率,kW;p为原油密度,kg/m3;H为扬程,m;Q为泵排量,3m/s。

再计入泵和电机的效率,则有:

油气管道能效管理

式中:N为电动机的输入功率,kW;η1为泵机组效率;η2为电动机效率。

所以t小时消耗的电量为

油气管道能效管理

t小时内,输送1万t原油1km的距离所消耗的电量:

油气管道能效管理

式中:SP为电耗,kW·h;SPP为电单耗,kW·h/(104t·km);H为扬程,m;L为管长,km。

从上式可知,由于周转量只与输量、距离有关,单位周转量电耗与运行时间无关。

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