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This report discusses the experiment conducted using a pipe friction apparatus and a hydraulic bench. The objectives of this experiment are twofold. First, to investigate the laws governing friction losses in pipe flows by measuring the friction factor as a function of the Reynolds number, considering both laminar and turbulent flows. Second, to experimentally determine the major losses due to friction in a fully developed pipe flow.
The following relations were utilized in the calculations of these experiments:
1. Reynolds Number:
The Reynolds number (Re) is calculated using the formula:
Re = ρuD/μ = uL/ν
Where,
2. Friction Factor (f):
The friction factor is determined from the following equation:
f = 4L/ρVD²g
Where,
The experiment was conducted in two parts.
In the first part, data such as pipe diameter, velocity, and area were collected to calculate the friction factor and Reynolds number, allowing us to investigate friction losses in pipes for both laminar and turbulent flow.
In the second part, a fully developed flow was established in the pipe, and the major losses due to friction were determined.
The apparatus used for this experiment included a Pipe Friction Apparatus, two manometers, and a hydraulic bench.
The Reynolds number is a dimensionless quantity that characterizes the nature of fluid flow within a pipe.
It is the ratio of inertial forces to viscous forces and predicts the flow regime of the fluid. A high Reynolds number indicates turbulent flow, while a low Reynolds number indicates laminar flow. Reynolds numbers falling between these extremes suggest transient flow.
For laminar flow, Re < 4000.
Where:
When Osborne Reynolds plotted the results of his investigation of energy head loss versus flow velocity, he identified two distinct regions separated by a transition zone. In the laminar region, the hydraulic gradient is directly proportional to the mean velocity, while in the turbulent flow region, the hydraulic gradient is proportional to the mean velocity raised to a power influenced by the roughness of the pipe wall. Smooth pipes, very rough pipes, and the transition region each have specific characteristics in terms of flow behavior.
The friction factor is a measure of the resistance to fluid flow and is influenced by the irregularities in the pipe's internal surface. Higher irregularities or roughness lead to greater friction. The Moody chart represents the friction factor as a function of the relative roughness (e/D) of the pipe against the Reynolds number. The chart distinguishes between flow in the wholly turbulent and laminar regions.
Roughness is a measure of irregularities along the boundary of the pipe's internal surface. It significantly affects the flow of the fluid passing through the pipe. Smooth-walled pipes promote smooth, laminar flow at low Reynolds numbers, while rough-walled pipes result in non-smooth, turbulent flow.
Volume (L) | Time (s) | Volumetric Flow Rate (L/s) | Volumetric Flow Rate (m³/s) | Density (kg/m³) | Area (m²) | Dynamic Viscosity (kg/m·s) | Velocity (m/s) |
---|---|---|---|---|---|---|---|
5 | 23.1 | 0.052756529 | 5.27565E-05 | 1000 | 9.25E-05 | 8.00E-04 | 1.581686037 |
5 | 24.2 | 0.097895252 | 9.78953E-05 | 1000 | 9.25E-05 | 8.00E-04 | 1.509791217 |
5 | 25.0 | 0.141043724 | 0.000141044 | 1000 | 9.25E-05 | 8.00E-04 | 1.461477898 |
5 | 25.1 | 0.169491525 | 0.000169492 | 1000 | 9.25E-05 | 8.00E-04 | 1.455655277 |
5 | 25.8 | 0.191204589 | 0.000191205 | 1000 | 9.25E-05 | 8.00E-04 | 1.416160754 |
Diameter (mm) | Kinematic Viscosity (m²/s) | h1 (m) | h2 (m) | hf (m) | Gravity (m/s²) | Length (m) | Reynolds Number | Friction Factor |
---|---|---|---|---|---|---|---|---|
10.86 | 8.00E-07 | 0.344 | 0.33 | 0.014 | 9.81 | 1 | 26097.8196 | 0.0346908 |
10.86 | 8.00E-07 | 0.36 | 0.3 | 0.06 | 9.81 | 1 | 24911.5551 | 0.0350517 |
10.86 | 8.00E-07 | 0.37 | 0.27 | 0.1 | 9.81 | 1 | 24114.3853 | 0.02063861 |
10.86 | 8.00E-07 | 0.386 | 0.22 | 0.166 | 9.81 | 1 | 24018.3121 | 0.01170228 |
10.86 | 8.00E-07 | 0.392 | 0.202 | 0.19 | 9.81 | 1 | 23366.6524 | 0.00412136 |
Friction factor = 0.315 * (2 * (9.81 / 1.581686037^2)) * (0.01086 / 1) = 0.0346908
Reynolds Number = (1.581686037 * 0.01086) / (8 * 10^(-7)) = 26097.8196
The purpose of this experiment is to calculate the Reynolds number and friction factor. To achieve this, various data points were collected, including:
All of these parameters were used in the calculations for both the Reynolds number and friction factor, making them essential experimental data.
A pipe with a diameter of 10.86 mm was used in the experiment. For this pipe, the Reynolds number ranged from 2.6E+4 to 2.3E+4, while the friction factor ranged from 3.48E-2 to 0.41E-2. A consistent trend is observed in both cases. As the Reynolds number decreases, the friction factor also decreases, indicating that laminar flow corresponds to lower Reynolds number values, resulting in lower friction factors. Conversely, as the Reynolds number increases, the friction factor also increases, indicating turbulent flow.
The transitional phase between laminar and turbulent flow is characterized by Reynolds numbers falling in this range, suggesting a transitional flow regime.
Several sources of error may have influenced the experimental results:
To minimize errors and improve the reliability of the results, the following suggestions can be considered:
For future experiments in this area, the following recommendations can be explored:
Reynolds Number | Friction Factor |
---|---|
26097.819607092897 | 3.4690860543329857E-2 |
24911.555079497768 | 3.5051716415518692E-2 |
24114.385316953845 | 2.063861547020689E-2 |
24018.312068679119 | 1.1702280719146535E-2 |
23366.652438908754 | 4.1213664004765508E-3 |
Experiment on Pipe Friction Apparatus & Hydraulic Bench. (2024, Jan 17). Retrieved from https://studymoose.com/document/experiment-on-pipe-friction-apparatus-hydraulic-bench
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