1) coal as received and coal as fired
入厂煤和入炉煤
1.
This paper gives a minute introduction of the present condition and existing problem of the sampling and preparation of coal as received and coal as fired at power plants in Anhui.
详细介绍了我省火电厂入厂煤和入炉煤的采样、制样现状和存在的问题。
2) coal as received
入厂煤
1.
Discussion on caloric differences betweencoal as received and coal as fired in power plant;
浅析火电厂入厂煤与入炉煤热值差异
2.
Design of Coal as Received Autosampling System Based on PLC
基于PLC的入厂煤自动采样系统设计
3.
Reasons analysis and countermeasure of caloric value differences between coal as received and coal as fired in thermal power plant
火电厂入厂煤与入炉煤热值差大的原因分析及对策
3) coal consumption entering furnace
入炉煤耗
4) coal as fired
入炉煤
1.
Discussion on caloric differences betweencoal as received and coal as fired in power plant;
浅析火电厂入厂煤与入炉煤热值差异
2.
Introduction for automatic coal-sampling equipment of CZ type used by coal as fired;
CZ型入炉煤自动采制样装置及使用
3.
Reasons analysis and countermeasure of caloric value differences between coal as received and coal as fired in thermal power plant
火电厂入厂煤与入炉煤热值差大的原因分析及对策
5) furnace coal weight
入炉煤量
1.
The method of furnace anti equity is adopted to measure the furnce efficiency because of the difficulty in gaining accurate furnace coal weight.
由于无法取得正确的入炉煤量 ,火电厂一般是采用锅炉反平衡法计算锅炉的正平衡效率。
补充资料：再入走廊
返回地球的航天器在再入大气层时必须经过的由两条不同高度的开普勒轨道所决定的区域。对于不限着陆区的再入走廊，可将航天器进入大气层时的速度换算成开普勒轨道(见二体问题)的近地点高度。近地点较高的一条开普勒轨道是再入走廊的上界，近地点较低的一条开普勒轨道为再入走廊的下界，两近地点高度之差为再入走廊的宽度。上界取决于航天器在近地点的速度（等于该点的环绕速度），下界取决于航天器允许承受的最大过载。近地点高于上界的轨道范围称为不可捕获区，近地点低于下界的轨道范围称为危险过载区。当航天器的速度小于上界近地点的环绕速度，航天器进入不可捕获区，在一圈之内不能返回地球。若航天器速度大于下界近地点的环绕速度，航天器进入危险过载区而损坏。当航天器速度位于这两个环绕速度之间，航天器进入再入走廊可安全返回地面。要求在预定区域着陆的再入走廊则复杂得多，这时要求再入走廊与着陆区域相连。为了进入再入走廊,航天器往往需要进行多次轨道修正。航天器的再入走廊与进入大气层时的速度和位置、航天器的气动外形、姿态机动的能力、允许过载的安全值、大气密度以及密度随高度的变化率、返回轨道等因素有关。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条