Volumetric flow rate

  1. Fluid dynamics


In physics and engineering, in particular fluid dynamics and hydrometry, the volumetric flow rate, (also known as volume flow rate, rate of fluid flow or volume velocity) is the volume of fluid which passes through a given surface per unit time. The SI unit is m3 s-1 (cubic meters per second). In US Customary Units and British Imperial Units, volumetric flow rate is often expressed as ft3/s (cubic feet per second). It is usually represented by the symbol Q.

Volumetric flow rate should not be confused with volumetric flux, as defined by Darcy's law and represented by the symbol q, with units of m3/(m2 s), that is, m s-1. The integration of a flux over an area gives the volumetric flow rate.

Fundamental definition

Fundamentally, the volume flow rate is defined as: [1]

\[ Q = \frac{\Delta V}{\Delta t} \] .

where:

  • Q = volumetric flow rate,
  • ΔV = change in volume flowing through the area,
  • Δt = time interval of volumetric flow.

In the limit ΔV and Δt become infinitesimally small, the algebraic definition becomes a calculus definition:

\[Q = \frac{{\rm d}V}{{\rm d}t}\]

Since this is only the time derivative of volume, a scalar quantity, the volumetric flow rate is also a scalar quantity. The change in volume is the amount that flows after crossing the boundary for some time duration, not simply the initial amount of volume at the boundary minus the final amount at the boundary, since the change in volume flowing through the area would be zero for steady flow (which isn't the case, since an amount of volume has passed the boundary in the time duration).

Useful definition

Volumetric flow rate can also be defined by:

\[ Q = \bold{v} \cdot \bold{A} \]

where:

The above equation is only true for flat, plane cross-sections. In general, including curved surfaces, the equation becomes a surface integral:

\[Q= \iint_A \bold{v} \cdot {\rm d}\bold{A} \]

This is the definition used in practice. The area required to calculate the volumetric flow rate is real or imaginary, flat or curved, either as a cross-sectional area or a surface. The vector area is a combination of the magnitude of the area through which the volume passes through, A, and a unit vector normal to the area, \(\bold{\hat{n}}\). The relation is \(\bold{A} = A \bold{\hat{n}}\).

The reason for the dot product is as follows. The only volume flowing through the cross-section is the amount normal to the area, i.e. parallel to the unit normal. This amount is: \[Q = v A \cos\theta \] where θ is the angle between the unit normal \(\bold{\hat{n}}\) and the velocity vector v of the substance elements. The amount passing through the cross-section is reduced by the factor \(\cos\theta \). As θ increases less volume passes through. Substance which passes tangential to the area, that is perpendicular to the unit normal, doesn't pass through the area. This occurs when θ = π/2 and so this amount of the volumetric flow rate is zero: \[Q = v A \cos(\pi/2) = 0\] These results are equivalent to the dot product between velocity and the normal direction to the area.

Related quantities

Volumetric flow rate is really just part of mass flow rate, since mass relates to volume via density.

See also

References

  1. ↑ http://www.engineersedge.com/fluid_flow/volumeetric_flow_rate.htm
cs:Objemový průtok

de:Volumenstrom es:Flujo volumétrico fa:نرخ جریان حجمی hr:Volumni protok he:ספיקה pl:Strumień objętości pt:Fluxo volumétrico ro:Debit volumic de curgere ru:Объёмный расход sk:Objemový prietok sl:Prostorninski pretok fi:Virtaama tr:Debi uk:Об’ємна витрата vi:Lưu lượng dòng chảy zh:體積流率


...