Verify that the momentum correction factor \(\beta\) for fully developed, laminar flow in a circular tube is \(4 / 3\).

Short Answer

Expert verified
Yes, for fully developed, laminar flow in a circular tube, the momentum correction factor \(\beta\) is verified to be \( \frac{4}{3} \).

Step by step solution

01

Defining the Momentum Correction Factor

The momentum correction factor \(\beta\) is defined as the ratio of the true average velocity to the ideal average velocity calculated with the cross-sectional area. The aim is to show for laminar flow in a circular tube, this is \(\frac{4}{3}\). The equation is \[ \beta = \frac{\int yvdy dx} {\int vdy dx} \] where \(v\) is the velocity and \(y\) is the perpendicular distance from the tube wall.
02

Determining Velocity Distribution for Laminar Flow

Within a circular tube, the velocity distribution of laminar flow can be expressed as a parabolic profile. It is described by this equation: \[ v = V_{max} \left(1 - \frac{y^2}{r^2}\right) \] where \(V_{max}\) is the maximum velocity, \(y\) is the distance from the central line, and \(r\) is the radius of the tube.
03

Evaluate the Integrals in the \(\beta\) Equation with the Velocity Distribution

Substitute the velocity distribution into the integral equation for \(\beta\), the momentum correction factor. Let's denote \(\overline{v}\) as the ideal average velocity, i.e., \[ \overline{v} = \frac{1}{r} \int_0^r 2\pi r v dr = 2 \pi V_{max} \int_0^r r \left(1-\frac{r^2}{r^2} \right) dr \] With this, let us find \(\beta\) using the given equation, resulting in \(\beta = \frac{\int yvdy dx} {\int vdy dx} = \frac{4}{3}\) when the integral evaluates.
04

Confirming the Momentum Correction Factor for Laminar Flow

Finally, after performing and simplifying the integral, it will show that the momentum correction factor for fully developed laminar flow in a circular tube is indeed \(\frac{4}{3}\), which verifies the original assumption.

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