CIVE2400-Flume Laboratory Handout

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    1

    University of Leeds

    Department of Civil Engineering

    Level 2 Fluid Mechanics Laboratory Class

    Critical Depth Flumes

    Objective

    The objective of this set of experiments is to demonstrate that when flow is made to pass

    through the critical depth a stable and reliable relationship exists which can be used to

    determine the flow in the channel. In order to create critical depth within the flow a structure

    has to be built in the channel. In this experiment three types of structure will be used, a broad

    crested weir, a Venturi flume and a simplified Crump weir.

    Theory

    The generalised equation for critical depth flumes will be derived in the lecture course, it can

    be written as

    Q 1.71Cd

    B(E1

    h)3 / 2

    where Q is the flow in m3/s

    1712

    3

    2

    3. is

    g in SI units

    Cdis a coefficient of discharge which should lie in the range 0.9 < C d < 1.0

    B is the width of the channel at the point where the depth is critical

    h is the height of the bed of the flume above the channel bed at the point where the

    flow is critical

    E1is the specific energy immediately upstream of the flume, this is defined as theenergy per unit weight of fluid using the bed of the channel as datum hence it has

    the dimensions of length and can be written as

    E yv

    1 1

    1

    2

    2g

    where y1is the depth of flow immediately upstream of the flume

    v1is the mean velocity of flow immediately upstream of the flume

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    2. Crump Weir

    Repeat the above experiment with the Crump weir.

    y1 Q E1-h (E1-h)3/2

    (m) (m3/sec) (m)

    Width of weir (B) = ______________(m)

    Height of weir (h) = _____________(m)

    3. The Venturi Flume

    The Venturi flume achieves the same effect as the weirs but by restricting the width instead ofraising the bed level.

    Place the two halves of the Venturi flume into the channel and hold it in position with the

    stretcher screw but be careful not fasten it too tightly otherwise you will split the sides of

    the flume. In this case the value of the height, h, in our generalised formula is zero however

    B has a value which is the width of the throat of the Venturi meter. Repeat the experiment

    with this flume.

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    y1 Q E1 E13/2

    (m) (m3/sec) (m)

    Width of flume (B) =______________(m)

    Graphs

    Plot the following graphs for each flume:-

    1. Q against (E1- h)3/2hence determine a value for Cd

    2. log Q against log (E1- h) hence determine both Cdand the power to which (E1- h)

    is raised. All the data for this graph will be far away from the origin; you should

    choose a scale so that the plot makes full use of the paper and then determine the

    intercept by similar triangles. If you choose scales so that the origin is on the paperthen the determination of the intercept will be grossly in error.

    After considering the results you should be able to answer the following questions

    how well does the equation relating flow to depth upstream of the

    flume describe what actually happens

    how well does the concept of a constant Cdmodel the energy loss

    whether or not critical depth actually occurs within the length of the

    flumes

    the effect of errors in the measurement of upstream depth on the

    computed value of the flow

    how effective the flumes are at very low flows

    how resistant the flumes are to flooding

    what can you say about the validity of the governing equation when flooding

    occurs

    If these flumes were being used to measure flow in a real river or water/sewage treatment

    works then what additional design considerations would you anticipate having to take into

    account?I.M. Goodwill.

    January, 2004.

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