# Velocity Patch in FDS

Created with software version 2020.1

## 1. Introduction

As part of exploring options to model jet fans (see our Jet Fan Tutorial), we looked at using a Velocity Patch. The FDS User Guide discusses the concept of a velocity patch in the context of air entrainment by the spray from a sprinkler nozzle. The idea is that the spray droplets accelerate the gas through which they move and a velocity patch gives a way to specify the gas velocity. We sought to apply a velocity patch to a model of a jet fan.

## 2. Velocity Patch Background

As described in the FDS User Manual (Section 15.3.3), “The details of the sprinkler head geometry and spray atomization are practically impossible to resolve in a fire calculation. As a result, the local gas phase entrainment by the sprinkler is difficult to predict. As an alternative, it is possible to specify the local gas velocity in the vicinity of the sprinkler nozzle.”

A velocity patch consists of:

1. A bounding volume
2. A cartesian point (XYZ)
3. Polynomial coefficients that define the velocity using a second order Taylor expansion about the cartesian point XYZ. The polynomial is specified by the coefficients:
• P0 - the value of the velocity component (k)
• PX(1:3) - the first derivatives at cartesian point XYZ
• PXX(1:3,1:3) - the second derivatives at cartesian point XYZ

If we want a constant velocity, we only specify P0. The first line of the FDS input in Figure 1 defines the velocity component (in this case the X direction) and the constant value, P0. The second line defines a timer that activates the patch. The third line defines the geometry of the patch and links the patch to the previous data. By default the point XYZ is the center of XB, but as will be shown below, you can add a point definition to this line to shift the center of the expansion.

For a parabolic velocity in the X direction that varies in the Y-Z plane, the Taylor expansion simplifies to:

The plot shows the velocity for a patch that extends from Y=-1 to Y=1 and Z=-1 to Z=1, with latex:[TCP_{mpp}] and $$P_{22}=P_{33}=-10$$. Figure 2. A parabolic velocity patch with the centerline velocity of 10 and 0 at the corners of the patch.

This was tested in PyroSim using the following FDS input data:

which resulted in the contours shown in Figure 4 that match the expected results. Figure 4. Test case for a parabolic velocity distribution with 10 at the centerline and 0 at the corners of the velocity patch.

To demonstrate shifting the XYZ point for the Taylor expansion from the center to the edge at Y=1, we add XYZ data to the velocity patch device:

This results in the countours shown in Figure 6: