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    Normal Hydraulic Jumps NHJ

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    28.1 Introduction

    When the depth of flow changes rapidly from a low stage to a high stage, it results in an

    abrupt rise of water surface. This local phenomenon is known as 'hydraulic jump'. It

    occurs in a canal below a regulating sluice, at the toe of a spillway or at the place where

    a steep channel slope suddenly turns flat. It is well known that a large amount of

    air entrains in the roller portion of the jump due to the breaking of the water surface.

    Consequently a large amount of energy loss occurs in the jump through dissipation in

    the turbulent body of water. A considerable amount of investigations, both theoretical

    and experimental, have been carried out on the jump (See box - History).

    SluiceGate

    1

    Hydraulic jump

    2

    3

    Fig. 28.1 - Rapidly varied flow with Hydraulic jump (1 and 3 subcritical flows,2 Super critical flow)

    Fig. 28.2 - Formation of Hydraulic jump at the toe of the spillway

    Hydraulic jump

    Toe

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    History

    The earliest description of the hydraulic jump appears to be by Leonardo da Vinci

    in 1452- 1519. Bidone was the pioneer to conduct investigations on the hydraulic

    jump in 1818 -1819. Belanger in 1828 developed the momentum equation

    connecting the sequent depths. Then onwards innumerable contributions have

    been made towards the understanding of the basic mechanism of the hydraulic

    jump. The following are some of the significant contributors amongst several

    investigators responsible for present state of knowledge of the jump: Bresse (

    1860 ), Darcy and Bazin ( 1865 ), Uniwin ( 1875 ), Ferriday and Merriman ( 1894

    ), Gibson ( 1913 ), Kennison ( 1916 ), Woodward and Riegel Beebe ( 1917 ),

    Koch and Cartstanjen ( 1926 ), Lindquist ( 1927 ), Safranez ( 1917 ), Einwachter

    ( 1933 ), Smetana ( 1934 ), Bakhmeteff and Matzke ( 1936 ) , Escande ( 1938 ),

    Citrini ( 1939 ), Nebbia ( 1940 ), Kindsvater (1944 ) , Blaisdell (1948 ), Forster

    and Skrinde (1950 ), Moore and Morgan ( 1957 ), and Rouse et al. (1958 ). A

    detailed mathematical treatment of hydraulic jump was made by Flores (1954 ) .

    Rajaratnam's contributions to the knowledge of hydraulic jumps during 1960s are

    outstanding. For a comprehensive bibliography on the jump, reference may be

    made to the following references: 'The standing wave or hydraulic jump ( 1950 ),

    (Central Board of Irrigation and Power)' ; ' A bibliography on hydraulic jump

    (Central Board of Irrigation and Power) ( 1955 )'; ' Hydraulic energy dissipators (

    1959 )' ( Elevatorski - The Hydraulic jump, May 1955); Hydraulic Energy

    dissipators Elevatorski - Mcgraw Hill, 1959) 'Open Channel Hydraulics Chow

    V.T., McGraw Hill ( 1959 )';'Advances in Hydroscience (Hydraulic jump byRajaratnam.N edited by Chow.V.T. Vol. - 4 , Academic Press New york and

    London, Page 197 to 280 ( 1967 )' ; Self Aerated flow characteristics in

    developing zones and in Hydraulic jumps, (Thandaveswara Phd Thesis, Indian

    Institute of Science, Bangalore, June- 1974).

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    Hydraulic Jump has many practical applications, for example (a) to dissipate the high

    kinetic energy of water near the toe of the spillway and to protect the bed and banks of

    a river near a hydraulic structure (b) to increase the head in the power channel (c) to

    remove air pockets from pipes (d) for mixing of chemical in water supply system.

    Figure below shows a schematic view of the classical hydraulic jump on a horizontal

    floor. The details in this unit are confined to the case of the hydraulic jumps on level

    floors in rectangular channels and this type of jump is referred to as the Normal

    Hydraulic Jump (NHJ). The supercritical Froude number of the approach flow is the

    major parameter that influences the characteristics of the hydraulic jump.

    L jLrj

    Toe

    1 2

    y2V2

    F1 y1 V1 y

    28.3 SCHEMATIC VIEW OF THE HYDRAULIC JUMP

    1 2

    x

    Hydrostatic pressure distribution Roller zone

    yr

    Super critical to sub critical