Pitot Tubes
Reference data and engineering information about pitot tubes for fluid mechanics applications.
Overview
Engineering reference data for Pitot Tubes in fluid mechanics.
Key Formulas
Reynolds Number
Ratio of inertial to viscous forces — determines flow regime.
Bernoulli's Equation
Conservation of energy for steady, inviscid, incompressible flow.
Continuity Equation
Conservation of mass for incompressible flow.
Darcy-Weisbach
Pressure drop due to friction in a pipe.
Variables
| Symbol | Description | Unit |
|---|---|---|
| Reynolds number | — | |
| Fluid density | kg/m³ | |
| Flow velocity | m/s | |
| Characteristic dimension | m | |
| Dynamic viscosity | Pa·s | |
| Pressure | Pa | |
| Darcy friction factor | — |
Key Formulas
The following equations are fundamental to pitot tube operation and flow measurement:
Pressure Definitions
Each term in the Bernoulli equation represents a specific type of pressure:
- Static Pressure (): The pressure relative to the moving fluid, measurable through a flat opening parallel to the flow.
- Dynamic Pressure (): The pressure component due to the fluid's kinetic energy.
- Hydrostatic Pressure ( or ): The pressure component due to the fluid's elevation, where is the specific weight.
Measurement & Application
The pitot tube measures the difference between total (stagnation) pressure at the tip and static pressure from the side ports. This pressure difference ( or ) is used with equations (4) or (5) to calculate the point velocity in the free stream.
For flow rate determination in a conduit, the point velocity-area method is used. Point velocities are measured across a traverse, and the average velocity () is calculated using equation (6). The volume flow () is then found from equation (7).
Practical Guidance:
- For round ducts larger than 10 inches (254 mm), a 10-point traverse is recommended at specific radial positions.
- For smaller ducts, the average velocity can be estimated as 81% of the centerline velocity.
- Pitot tubes are not suited for low-velocity flows due to the small dynamic pressure differential, which leads to inaccurate readings.