# Steady Flow Devices

A **steady flow device** is any device that will have a continuous flow of material through it. Some examples of steady flow devices include pipes, nozzles, diffusers, and pumps. Generally the material flowing through the device is a gas or liquid, and if the device in any way changes the velocity of the fluid then that fluid will exert a force on the steady flow device in return.

In order to determine the forces at play on a steady flow device, we will start with our impulse and momentum equation.

\[\vec{J} = m \vec{v_{f}}-m \vec{v_{i}}\] |

Because this is a continuous process, it doesn't really make sense to have initial and final velocities. Instead we will have an inlet and outlet velocities. Also, the mass will need to be changed to the mass flow rate (the mass entering or leaving the device per unit time) to deal with the continuous flow nature of the system.

Dividing our initial impulse-momentum equation by time on both sides will give us the desired mass flow rate on the right, while the time on the left will cancel out the time component of the impulse.

\[\frac{\vec{F}*t}{t} = \frac{m_{out}}{t} \vec{v_{out}}-\frac{m_{in}}{t} \vec{v_{in}}\] |

Simplifying this equation we will arrive at our final equation, which relates the force our steady flow device exerts on the fluid to the mass flow rates and velocities at the inlet and outlet. The force the fluid exerts on the device would simply be equal and opposite to the force below.

\[\vec{F} = \dot{m}_{out} \vec{v_{out}}-\dot{m}_{in} \vec{v_{in}}\] |

One final note is that these equations are vector equations. If the device is changing the direction of the flow of a fluid you will need to break the force and velocities into x and y components and split the above equation into x and y components.

## Finding Mass Flow Rate:

If the mass flow rate in or out of your device is not given directly, you may need to find those values. First we can use a simple identity, knowing the mass flow rate will be equal to the density of the fluid times the volumetric flow rate. Furthermore, the volumetric flow rate can be related to the geometry of the device, in that it will be equal to the average velocity of the fluid at the inlet or outlet times the cross sectional area at the inlet or outlet. Putting this all together, we arrive at the following formulas.

\[\dot{m}= \rho \dot{V} = \rho \vec{v} A\] |