Design and measurement error estimation of a shielded total temperature probe
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摘要:
在忽略辐射误差的情况下,使用流固耦合传热数值模拟的方法预测了一种总温探头在不同工况下的速度误差和导热误差。结果表明:在马赫数为0.2~0.6的范围内,导热误差都保持在较小值;总误差的90%以上由速度误差贡献;最大测量误差为1.13 K,比结构A、结构B、结构C以及结构D分别低了331.6%、119.4%、61.6%以及59.5%;速度误差和导热误差存在互相影响的关系,存在最优解可使总误差最小;适用于等温来流和马赫数大于0.5的高速非等温来流的总温测量。最后探讨了热电偶节点位置对测量精度的影响,节点在从设计点远离支持体的过程中,测量误差遵循着先增大后减小的变化规律。
Abstract:Ignoring the radiation error, the velocity error and heat conduction error of a shielded total temperature probe under different working conditions were predicted by using the conjugate heat transfer numerical simulation method. Results showed that the thermal conductivity error was kept at a small value in the range of Mach number from 0.2 to 0.6; more than 90% of the total error was contributed by velocity error; the maximum measurement error was 1.13 K, which was 331.62%, 119.4%, 61.6% and 59.5% lower than the common structure A, B, C and D, respectively; velocity error and conduction error affected each other, and there was an optimal solution to minimize the total error. It was applicable to the total temperature measurement of isothermal incoming flow and high-speed non-isothermal incoming flow with Mach number greater than 0.5. Finally, the influence of thermocouple junction position on measurement accuracy was discussed. When the junction was kept away from the support from the design point, the measurement error followed the change law of first increasing and then decreasing.
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表 1 网格无关性验证
Table 1. Verification of grid independence
网格名称 网格数/万 Tj/K 第1套 314 338.75 第2套 467 338.59 第3套 628 338.57 表 2 仿真工况
Table 2. Simulation conditions
工况 $ {V}_{\mathrm{i}\mathrm{n}} $ $ {T}_{\mathrm{s}} $/K $ {p}_{\mathrm{o}\mathrm{u}\mathrm{t}} $/Pa A Ma=0.2 B Ma=0.3 C Ma=0.4 323.15 101325 D Ma=0.5 E Ma=0.6 表 3 使用Moffat误差估计公式对裸线式热电偶测量误差进行估计的结果
Table 3. Estimation results of measurement error of bare wire thermocouple using Moffat error estimation formula
Ma ${T}_{\mathrm{j} }/{\rm{K}}$ $ {T}_{0}/{\rm{K}} $ $ {E}_{\mathrm{v}}/{\rm{K}} $ $ {E}_{\mathrm{c}}/{\rm{K}} $ $ {E}_{\mathrm{r}}/{\rm{K}} $ $ E/{\rm{K}} $ 0.2 325.1 325.7 $ 0.65~1.00 $ $ 0.38~0.44 $ $0.002\;1~0.002\;8$ $ 1.03~1.45 $ 0.3 327.5 329.0 $ 1.45~2.68 $ $ 0.76~0.89 $ $0.003\;7~0.004\;9$ $ 2.21~3.16 $ 0.4 330.9 333.5 $ 2.59~4.03 $ $ 1.21~1.45 $ $0.005\;7~0.007\;6$ $ 3.80~5.49 $ 0.5 353.3 339.3 $ 4.04~6.30 $ $ 1.72~2.09 $ $0.008\;1~0.011\;0$ $ 5.77~8.40 $ 0.6 340.6 346.4 $ 5.82~9.07 $ $ 2.25~2.78 $ $0.011\;0~0.015\;0$ $ 8.08~11.86 $ 名称 材料 导热系数/
$(\mathrm{W}/ (\mathrm{m}\cdot \mathrm{K}) )$发射率 屏蔽罩 不锈钢 15 0.85 左偶丝 镍硅合金 29.71 0.9 右偶丝 镍硅合金 19.25 0.9 偶丝节点 24.48 0.9 支持体 尼龙 0.2 0.1 表 5 3种改型偶丝的长度和直径
Table 5. Length and diameter of three modified wires
型号 偶丝长/mm 偶丝直径/mm 长径比 原型 1.7 0.3 5.67 改型1 2.4 0.3 8 改型2 2.4 0.15 16 改型3 3.1 0.3 9.3 表 6 改型后3种屏蔽式总温热电偶在Ma=0.6时的误差组成及增量百分比
Table 6. Error composition and increment percentage of three shielded total temperature thermocouples after modification when Ma=0.6
型号 $ {E}_{\mathrm{c}}/{\rm{K}} $ ${\delta }_{\mathrm{c} }/{\text{%}}$ $ {E}_{\mathrm{v}}/{\rm{K}} $ ${\delta }_{\mathrm{v} }/{\text{%}}$ $ E/{\rm{K}} $ $\delta /{\text{%}}$ 原型 0.115 1.014 1.129 1 0.048 −56.5 1.306 28.8 1.356 20.1 2 0.077 −33.0 1.221 20.4 1.298 15.0 3 0.091 −20.9 1.126 11.0 1.035 −8.3 -
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