Start with the measurand and reference planes
Two 仪表 connected to one static fluid system can experience different 压力s at different elevations. Beamex's 压力-表压 校准 guidance identifies height difference as a source of hydrostatic error, particularly with liquids.
Call the measurement reference R and the device under test D. Use their manufacturer-defined 压力-reference planes. Let z increase upwards and define delta_z = z_D - z_R. This definition must accompany a correction; a height magnitude alone does not specify its sign.
A static model with explicit limits
For a single connected fluid of effectively constant density at rest, the 绝压-压力 relation is p_D_abs = p_R_abs - rho_fluid × g × delta_z. Here density is in kg/m³, g in m/s², height in m and 压力 in Pa.
For two 表压-压力 measurements locally referenced to the same surrounding atmosphere, with effectively constant fluid and air densities over the height difference, the corresponding relation is p_D_表压 = p_R_表压 - (rho_fluid - rho_air) × g × delta_z. Appendix A2.2 of the BIPM-hosted EURAMET.M.P-S14 report provides a 表压-压力 head-correction model including fluid minus air density. Its height convention is opposite to delta_z as defined here.
These are static teaching models, not a universal 校准 procedure. 差压-压力仪表, mixed fluid columns, 压力-dependent density and different reference arrangements need their own documented treatment. A gas head is not automatically negligible for every uncertainty target.
Worked example: D is above R
Assume 表压 压力 at R = 100 kPa, rho_fluid = 1000 kg/m³, rho_air = 1.2 kg/m³, g = 9.80665 m/s² and delta_z = +0.30 m. These are hypothetical inputs, not measured fluid properties or WESIVO specifications.
- The positive head magnitude is (1000 - 1.2) × 9.80665 × 0.30 = 2938.464606 Pa, approximately 2.938 kPa.
- With D above R, 压力 at D is approximately 97.062 kPa 表压.
- With D instead 0.30 m below R, delta_z is negative and 压力 at D is approximately 102.938 kPa 表压.
- At equal reference-plane elevations, this idealised height term is zero; other errors and uncertainties remain.
The corrected reference value at D is the comparison input. It is not the DUT indication error by itself. Determine that error by comparing the DUT indication with the appropriately corrected reference value, following the chosen procedure and sign convention.
Keep the correction auditable
Record both reference-plane identities, signed height and units, fluid and density basis, applicable conditions, 压力 type, equation convention, correction and the uncertainty treatment. EURAMET cg-17 v4.1 includes consideration of uncertainty associated with estimated head correction. Do not replace a documented geometry correction with an unexplained zero adjustment.
Use the density appropriate to the fluid and measurement conditions; the assumed value above is not a universal water or oil density. Have the responsible metrologist decide which effects are significant for the actual range and target uncertainty.
Equipment 选型 is a separate decision
The WESIVO 880 product page and original datasheet support a configuration enquiry. Confirm the ordered 压力 type and range, reference 液位, applicable certificate and intended role. No automatic head-correction capability is asserted here.
The related 522U pump is a 压力-source listing, not a recommendation for this 100 kPa teaching example. Neither the calculation nor these product links establish a validated equipment combination. Send the actual setup drawing and measurement requirements when requesting a quotation.
先确定被测量和压力基准面
即使连接在同一个静止流体系统中,两台仪表位于不同高度时,也可能承受不同的压力。Beamex 的压力表校准说明将高度差列为静压误差来源,尤其需要关注液体介质。
用 R 表示参考仪表、D 表示被校仪表,采用制造商定义的压力基准面。令垂直坐标 z 向上为正,定义 delta_z = z_D - z_R。修正记录必须同时保留这个定义,仅有高度差的绝对值不能确定修正方向。
明确边界的静态模型
对于连通、静止且密度可视为常数的单一流体,绝对压力关系为 p_D_abs = p_R_abs - rho_fluid × g × delta_z。密度单位为 kg/m³,g 为 m/s²,高度为 m,压力为 Pa。
若两台表压仪表各自在当地参考同一个周围大气,且流体和空气密度在该高度差内可视为常数,则相应关系为 p_D_表压 = p_R_表压 - (rho_fluid - rho_air) × g × delta_z。BIPM 收录的 EURAMET.M.P-S14 报告附录 A2.2 给出了包含“流体密度减空气密度”的表压高度差模型;该报告的高度正方向与本文 delta_z 的定义相反。
以上是静态教学模型,不是适用所有校准装置的程序。差压仪表、混合液柱、随压力变化的密度和其他参考方式需要分别建立有依据的处理方法。气体静压影响也不能对所有不确定度目标一律忽略。
算例:被校仪表 D 高于参考仪表 R
假设 R 处表压为 100 kPa,rho_fluid = 1000 kg/m³,rho_air = 1.2 kg/m³,g = 9.80665 m/s²,delta_z = +0.30 m。这些是教学假设,不是实测介质性质或 WESIVO 产品参数。
- 正的高度差影响量为 (1000 - 1.2) × 9.80665 × 0.30 = 2938.464606 Pa,约为 2.938 kPa。
- D 高于 R 时,D 处表压约为 97.062 kPa。
- 若改为 D 低于 R 0.30 m,delta_z 为负,D 处表压约为 102.938 kPa。
- 两个压力基准面等高时,这个理想化高度项为零,其他误差和不确定度仍然存在。
换算到 D 处的参考压力才是比较输入,高度差修正本身不是被校仪表示值误差。应按选定程序和符号约定,将被校仪表示值与正确修正后的参考值比较,再确定示值误差。
保留可复核的修正记录
记录两台仪表的压力基准面定义、带正负号的高度及单位、流体与密度依据、适用条件、压力类型、公式约定、修正值和不确定度处理。EURAMET cg-17 v4.1 包括对估计高度差修正相关不确定度的考虑。不能用没有说明的调零代替有记录的几何修正。
应使用与实际流体和测量条件相符的密度,上面的假设值不能作为所有水或油的通用密度。由负责计量人员判断哪些影响对实际量程和目标不确定度显著。
设备选型需要另行判断
WESIVO 880 产品页与原版资料可用于发起配置询价,实际订购的压力类型、量程、压力基准位置、适用证书和用途均需确认。本文没有宣称该产品具备自动高度差修正功能。
相关 522U 产品属于压力源信息,不是针对上述 100 kPa 教学算例的设备推荐。本算例和产品链接都不能证明设备组合已经验证。询价时请提供实际装置图和测量要求。
沟通您的应用需求
请提供介质、工况、连接、输出、数量及收货地区,WESIVO 将在报价前核对配置。