The risk assessment for this laboratory can be found in SARAH, RA 24757. All students attending laboratory sessions on-campus are required to familiarize themselves with this document and follow the protocols/safe work instructions within it.
This laboratory session will use a range of working sections to break down and teach the concepts of the Energy equation and implement them in practice. The Energy Equation is similar to Beroulli’s equation but incorporates terms to account for viscous losses (hl) and energy added to the flow (hg).

Energy equation where is the pressure (Pa), is the fluid density (kg/m3), V is the velocity (m/s), is the gravitational acceleration (m/s2), is the height above a reference point (m), hl is the head loss (m) and hg is the head gain (m).
Another useful equation is the Continuity Equation which describes that the mass of the system must remain constant over time and since this system is a closed loop of water, the total flow rate will remain the same within the flow loop.

Continuity equation where is the fluid density (kg/m3), A is the cross-sectional area and V is the area normal flow velocity (m/s)
The experimental apparatus offers the ability to measure pressures at various points in the flow. Pressure losses will occur throughout the system due to viscous effects (flow disturbance, flow separation, friction etc.). These losses can be categorized as major or minor losses.
Major losses occur due to viscous effects in straight sections of pipe (note we will assume that the flexible tubing used in this laboratory can be approximated as straight). The pressure head loss in a constant diameter section due to major losses is given by the Darcy-Weisbach equation:

Darcy-Weisbach major loss equation where hL major is the pressure head loss (m), f is the dimensionless friction factor, L is the length over which the loss occurs (m), D is the diameter (m), V is the velocity (m/s) and g is gravity.
The friction factor f can be calculated from the Colebrook equation or read from a Moody chart and is a function of the dimensionless parameters Reynolds number ReD and relative surface roughness of the pipe e/D.
Minor losses occur due to components of the system that disturb the flow e.g. valves, elbows, T-pieces etc. The flow through these components is complex. Rather than attempting to calculate the losses theoretically the pressure loss is described using an empirical loss coefficient. The pressure head loss due to minor losses in an individual component is given by:

The results for these pre-lab questions should be entered into an online quiz which will close 10minutes before the start of the first Energy lab regardless of your allocated lab time.
1. Flow either side of a t-piece is shown in Figure 1. All flows are in the horizontal plane. Pitot tube flow meters with pressure measurements are fitted to two of the branches (top and RHS) while the other branch (LHS) has a sudden flow contraction. Pressures are measured at 4 points (labelled 1-4). The loss coefficient of the contraction connector KL,cc is known but the loss coefficient of the T-piece KL,TP is not. The known values are given in Table 2. In your calculations use 1000 kg/m3 as the density of water.

Calculate the following (you may assume major losses are negligible):
2. Flow either side of a t-piece is shown in Figure 2. All flows are in the horizontal plane. A pressure tapping gives the pressure of the flow coming into the left side of the T-piece. The known values are given in Table 3. In your calculations use 1000 kg/m3 as the density of water.

The assessment focuses on applying fluid mechanics principles in a laboratory setting, specifically using the Energy Equation and Continuity Equation to analyze flow in a closed water system. Students are required to:
The Academic mentor guided the student through the assessment in a structured process:
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