A method and device for measuring fluid velocity based on convective heat transfer
A technology of fluid flow rate and convective heat transfer, which is applied in the direction of measuring fluid velocity by using thermal variables, which can solve the problems of easy breakage of hot wires, influence on the accuracy of measurement results, interference, etc., and achieve accurate measurement results
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Embodiment 1
[0047] When the part where the measuring probe is in contact with the measured fluid is a plate structure, the following heat transfer formula is listed:
[0048]
[0049]
[0050]
[0051]
[0052] Among them: Pr is the Prandtl number, ν is the kinematic viscosity, λ is the thermal conductivity, L is the measuring probe,
[0053] For steady-state heat transfer, due to the critical Reynolds number Re cis a constant, and for a specific fluid, Prandtl number Pr, kinematic viscosity ν and thermal conductivity λ are only related to temperature, so Prandtl number Pr, kinematic viscosity ν and thermal conductivity λ can be calculated according to T k and T w Obtained, the length L of the measuring probe is known, combined with formulas (1), (2), and (3), we can get That is, the fluid flow rate u corresponds to the heat transfer coefficient h one by one, and the formula (4) is brought into the formula Since the heat transfer area A of the measuring probe and the meas...
Embodiment 2
[0055] When the part where the measuring probe is in contact with the measured fluid is a circular tube structure, the following heat transfer formula is listed:
[0056] Nu m =CRe n PR 1 / 3 (1)
[0057]
[0058]
[0059]
[0060] Among them: Pr is the Prandtl number, ν is the kinematic viscosity, λ is the thermal conductivity, L is the measuring probe, C and n are known constants that can be obtained by looking up the table according to the range of Re;
[0061] The fluid velocity u is calculated by formulas (1), (2), (3), and (4).
Embodiment 3
[0063] When the part of the measuring probe in contact with the measured fluid is a spherical structure, the following heat transfer formula is listed:
[0064]
[0065]
[0066]
[0067]
[0068] Among them: Pr is the Prandtl number, ν is the kinematic viscosity, λ is the thermal conductivity, L is the measuring probe, η k For the measured fluid at temperature T k Dynamic viscosity at , η w For the measured fluid at the wall temperature of the measuring probe T w The dynamic viscosity under , and when the measured fluid type and temperature are known, then η k and η w is a known constant.
[0069] The fluid velocity u is calculated by formulas (1), (2), (3), and (4).
[0070] In addition, in step S3, when the heat transfer between the measuring probe and the measured fluid is a steady-state heat transfer, specifically: within a ΔT time, T k The temperature is constant and the input cooling fluid enters the temperature T of the measuring probe 0 constant.
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