These directions replace the previous design directions of the same number, without amendment. The values presented there were revised for this edition and a chapter was added for shaft shiftings. 这些说明取代了之前相同编号的设计说明,未作任何修改。本版对其中的数值进行了修订,并增加了关于轴移位的章节。
These directions comprise half-speed ( 1500min^(-1)1500 \mathrm{~min}^{-1} and 1800min^(-1)1800 \mathrm{~min}^{-1} ), and full-speed ( 3000min^(-1)3000 \mathrm{~min}^{-1} and 3600min^(-1)3600 \mathrm{~min}^{-1} ) bearings of 280-:900mm280 \div 900 \mathrm{~mm} diameters. The data required for the layout of the 3 -segment standard journal bearings have been established. Energy losses, oil needs, oil-heating, and admissible maximal bearing loads are presented as a function of the diameter for the entire diameter range. The shaft shiftings can be determined for the entire diameter and rotational speed ranges. 这些方向包括直径为 280-:900mm280 \div 900 \mathrm{~mm} 的半速( 1500min^(-1)1500 \mathrm{~min}^{-1} 和 1800min^(-1)1800 \mathrm{~min}^{-1} )和全速( 3000min^(-1)3000 \mathrm{~min}^{-1} 和 3600min^(-1)3600 \mathrm{~min}^{-1} )轴承。3 段标准轴颈轴承布局所需的数据已经确定。在整个直径范围内,能量损失、机油需求、机油加热和允许的最大轴承载荷与直径相关。可以确定整个直径和转速范围内的轴偏移。
2. Object 2.对象
Fully enclosed journal bearings with a diameter of d >= 400mmd \geq 400 \mathrm{~mm} enter the area of turbulent bearing friction at or above 3000min^(-1)3000 \mathrm{~min}^{-1} under the usual BBC operating conditions. The resulting heavy increase in bearing losses can be controlled by the use of segment bearings. In addition, segment bearings show excellent stabilizing properties. The use of segment journal bearings is treated in HTGD 662014. 直径为 d >= 400mmd \geq 400 \mathrm{~mm} 的全封闭轴颈轴承在通常的BBC工作条件下,当直径达到或超过 3000min^(-1)3000 \mathrm{~min}^{-1} 时,就会进入轴承摩擦湍流区。由此造成的轴承损耗的严重增加可以通过使用分段轴承来控制。此外,分段轴承还具有优异的稳定特性。HTGD 662014对分段轴颈轴承的使用进行了研究。
3. Bearing data sheet records 3.轴承数据表记录
Observe the following when filling in the data sheets: 填写数据表时请注意以下几点:
3.1 Clearance 3.1 清理
The manufacturing clearance of the segments, psi_(S)\psi_{S}, is 1.5%1.5 \% for all 3 SL. The adjusting clearance of the bearing psi_(e)\psi_{e} (designated with “v” in the operating instructions) is 0.8 - 1.0%1.0 \% for the half-speed ( 1500min^(-1)1500 \mathrm{~min}^{-1} and 1800min^(-1)1800 \mathrm{~min}^{-1} ) bearings of diameters >= 600mm\geq 600 \mathrm{~mm}. For all the other bearings, full-speed and half-speed ( 3600min^(-1)3600 \mathrm{~min}^{-1} and 3000min^(-1)3000 \mathrm{~min}^{-1}, as well as 1800min^(-1)1800 \mathrm{~min}^{-1} and 1500min^(-1)1500 \mathrm{~min}^{-1} ), the adjusting clearances psi_(e)=0.15%\psi_{e}=0.15 \% to 0.35%0.35 \%. 对于所有 3 个 SL,分段的制造间隙 psi_(S)\psi_{S} 为 1.5%1.5 \% 。对于直径为 >= 600mm\geq 600 \mathrm{~mm} 的半速( 1500min^(-1)1500 \mathrm{~min}^{-1} 和 1800min^(-1)1800 \mathrm{~min}^{-1} )轴承, psi_(e)\psi_{e} (操作说明书中用 "v "表示)的调整游隙为 0.8 - 1.0%1.0 \% 。对于所有其他轴承,全速和半速( 3600min^(-1)3600 \mathrm{~min}^{-1} 和 3000min^(-1)3000 \mathrm{~min}^{-1} 以及 1800min^(-1)1800 \mathrm{~min}^{-1} 和 1500min^(-1)1500 \mathrm{~min}^{-1} ),调整间隙为 psi_(e)=0.15%\psi_{e}=0.15 \% 至 0.35%0.35 \% 。
3.2 Load 3.2 装载
The specific load p_(m)p_{m} refers to the surface, i.e. bearing diameter times journal bearing width, as for fully enclosed bearings. 比载荷 p_(m)p_{m} 是指表面,即轴承直径乘以轴颈轴承宽度,与全封闭轴承相同。
specific load 特定负载
p_(m)=(F)/((b)*(d))" in "N//mm^(2)p_{m}=\frac{\mathrm{F}}{\mathrm{~b} \cdot \mathrm{~d}} \text { in } \mathrm{N} / \mathrm{mm}^{2}
F="="F \xlongequal{=} bearing load in NN NN 中的 F="="F \xlongequal{=} 轴承载荷 b=b= bearing segment width in mm b=b= 轴承段宽度(毫米
d 今 bearing diameter in mm d 今 轴承直径(毫米
The diagram sheets HTGD 41 043/1-6 of the directions were calculated, based upon a p_(m)=2.8N//mm^(2)p_{m}=2.8 \mathrm{~N} / \mathrm{mm}^{2} load. 图纸 HTGD 41 043/1-6 的方向是根据 p_(m)=2.8N//mm^(2)p_{m}=2.8 \mathrm{~N} / \mathrm{mm}^{2} 负载计算得出的。
The maximally admissible load p_(m)p_{m} can be read from the sheet HTGD 41043//541043 / 5. The maximum bearing metal temperature to be expected at P_(m" max. ")\mathrm{P}_{\mathrm{m} \text { max. }} is T_(WM)^(max)\mathrm{T}_{\mathrm{WM}}^{\max }. =12^(@)C=12^{\circ} \mathrm{C}. 最大允许载荷 p_(m)p_{m} 可从 HTGD 41043//541043 / 5 表中读取。在 P_(m" max. ")\mathrm{P}_{\mathrm{m} \text { max. }} 时,预计轴承金属的最高温度为 T_(WM)^(max)\mathrm{T}_{\mathrm{WM}}^{\max } . =12^(@)C=12^{\circ} \mathrm{C} .
3.3 Energy loss 3.3 能量损失
The energy loss Deltap\Delta \mathrm{p} refers to p_(m)=2.8N//mm^(2)\mathrm{p}_{\mathrm{m}}=2.8 \mathrm{~N} / \mathrm{mm}^{2} and is presented in HTGD 41 043/1. For other loads (deviating from this value) the energy loss must be corrected by a factor k_(p)pk_{p} p as per HTGD 41 043/3, whereby 能量损失 Deltap\Delta \mathrm{p} 指的是 p_(m)=2.8N//mm^(2)\mathrm{p}_{\mathrm{m}}=2.8 \mathrm{~N} / \mathrm{mm}^{2} 并在 HTGD 41 043/1 中列出。对于其他负载(偏离该值),能量损失必须按照 HTGD 41 043/3 以系数 k_(p)pk_{p} p 进行修正,即
energy loss: quad p=k_(p)p*Delta p quad\quad p=k_{p} p \cdot \Delta p \quad in kWk W 能量损失: quad p=k_(p)p*Delta p quad\quad p=k_{p} p \cdot \Delta p \quad 中的 kWk W
3.4 Oil flow 3.4 油流
The oil flow DeltaV^(˙)\Delta \dot{V} required by the bearing is presented on sheet HTGD 41 043/2. It refers to the specific load of 2.8N//mm^(2)2.8 \mathrm{~N} / \mathrm{mm}^{2}. For deviating load values the oil flow is corrected by the factor k_(pV^(˙))k_{p \dot{V}} as per HTGD 41043//341043 / 3, whereby the 轴承所需的油量 DeltaV^(˙)\Delta \dot{V} 见 HTGD 41 043/2 表。它指的是 2.8N//mm^(2)2.8 \mathrm{~N} / \mathrm{mm}^{2} 的特定载荷。对于偏差的载荷值,油流量将根据 HTGD 41043//341043 / 3 的系数 k_(pV^(˙))k_{p \dot{V}} 进行修正,从而得到DeltaV^(˙)\Delta \dot{V}。
" oil flow "quadV^(˙)=k_(pV^(˙))*DeltaV^(˙).quad" in "1//s\text { oil flow } \quad \dot{V}=k_{p \dot{V}} \cdot \Delta \dot{V} . \quad \text { in } 1 / s