12
Seoul National University 457.309.02 Hydraulics and Laboratory . 09 Turbulent flow in rough pipe Prepared by Jin Hwan Hwang (2019.04.03 )

457.309.02 Hydraulics and Laboratory .09Turbulent flow in rough pipe · 2019. 9. 3. · 457.309.02 Hydraulics and Laboratory.09Turbulent flow in rough pipe Prepared by Jin Hwan Hwang

  • Upload
    others

  • View
    1

  • Download
    0

Embed Size (px)

Citation preview

  • Seoul National University

    457.309.02 Hydraulics and Laboratory

    .09 Turbulent flow in rough pipe

    Prepared by Jin Hwan Hwang(2019.04.03)

  • Seoul National University

    Today’s objectives

    § Similarly to the smooth pipe case, turbulent flow in rough pipe will be understood.

    § Classifying the pipes whether they are smooth or rough§ Evaluating pipe friction factors in the given condition

    2

  • Seoul National University

    § Pipe friction in rough pipe will be governed by the size and patterns of the roughness (like as sediment particles)

    § As we learned through the last class, velocity profile follows logarithm no matter what flow is laminar or turbulent.

    § When roughness is high, the viscous layer will be canceled and viscosity may not be the important parameter.

    § Experiment proved that the viscosity can be replaced by the roughness in the rough wall condition.

    § In this condition Q (flow rate) can be determined as

    Turbulent flow – Rough pipes

    3

    uu*

    = 5.75 log ye+ 8.5 (Rough pipe, when e is roughness)

    Q = u(2πr dr)0

    R

    ∫ = 2πu* 5.75 logR − re

    ⎛⎝⎜

    ⎞⎠⎟ + 8.5

    ⎡⎣⎢

    ⎤⎦⎥r dr

    0

    R

  • Seoul National University

    § Therefore, the mean velocity is

    § Since

    § With experimental adjustment,

    Rough pipes’ friction factor

    Turbulent flow – Rough pipes

    4

    Vu*

    = 5.75 log Re+ 4.75

    u* =Vf8

    1f= 2.03log R

    e+1.68

    1f= 2.0 log d

    e+1.14

  • Seoul National University

    § The mean velocity in a 300 mm pipeline is 3m/s. The relative roughness of the pipe is 0.002 and the kinematic viscosity of the water is 9 x 10-7 m2/s. Determine the friction factor, the centerline velocity, the velocity 50 mm from the pipe wall, and the head lost in 300 m of this pipe under the assumption that the pipe is rough.

    – Friction factor– Centerline velocity– The velocity at 50 mm from the wall– Head loss

    Example

    5

  • Seoul National University

    – Friction factor

    – Centerline velocity

    – The velocity at 50 mm from the wall

    – Head loss

    Example

    6

    1f= 2.0 log d

    e+1.14

    ucu*

    = 5.75 log Re+ 8.5, u* =V

    f8

    u50u*

    = 5.75 log y50e

    + 8.5

    hL = fldV 2

    2gn

  • Seoul National University

    § What parameters do we need to compare to know whether flow is smooth or rough?

    § To cancel this, we need to see the ratio between this and that.– This is viscous sublayer thickness and roughness height

    § What is the viscous sublayer thickness in Laminar flow?– Since viscosity governs overall depth in pipe, R should be the thickness.– Therefore, in a Laminar flow, no matter what smooth or rough,

    § In turbulent flow,

    Classification of smoothness and roughness

    7

    f = 64Re

    eδν

    = e / dδν / d

    = e / d32.8 / Re f

    = ed

    ⎛⎝⎜

    ⎞⎠⎟Re f32.8

    edRe f = 32.8 e

    δν

  • Seoul National University

    § Now we can plot the results with

    Classification of smoothness and roughness

    8

    edRe f and 1

    f− 2.0 log d

    e

    1f− 2.0 log d

    e= 1.14

    Fully rough flow

    1f= 2.0 log Re f( )− 0.8

    1f− 2.0 log d

    e= 2.0 log e

    dRe f⎛⎝⎜

    ⎞⎠⎟ − 0.8

    Smooth flow

    1f− 2.0 log d

    e= 1.14 − 2log 1+ 9.28

    Re(e / d) f⎡

    ⎣⎢

    ⎦⎥ (For commertial highly turbulent flow)

  • Seoul National University

    § Classifications

    Classification of smoothness and roughness

    9

    For smooth flow: ed

    Re f ≤10

    For transition flow: 10< ed

    Re f < 200

    For rough flow: 200 ≤ ed

    Re f

  • Seoul National University

    Classification based on velocity profile

    § Another means of classification of the roughness effects is to use the velocity profiles directly. In all pipes (page 331),

    § In rough pipes,

    10

    uc − uu*

    = 5.75 log Ry

    uu*

    = 5.75 log ye+ 8.5

    ucu*

    = 5.75 log Re+ 8.5 (At center)

    uc − uu*

    = 5.75 log Re− log y

    e⎛⎝⎜

    ⎞⎠⎟

    = 5.75 log Ry

  • Seoul National University

    Classification based on velocity profile

    § Now let’s modify the equation – For both (smooth and rough)

    § In smooth flow, A=8.5 from experiment.§ Check the page 332, equation 9.17,

    11

    uu*

    = ucu*

    + 5.75 log yR

    = ucu*

    + 5.75 log eR+ 5.75 log y

    e

    = A + 5.75 log ye

    A = ucu*

    + 5.75 log eR

    uu*

    = 5.75 log u*yν

    + 5.5 (Smooth pipe)

    = 5.5 + 5.75 log u*eν

    + 5.75 log ye

    = A + 5.75 log ye

    A = 5.5 + 5.75 log u*eν

  • Seoul National University

    Classification based on velocity profile

    § In the previous equation is the Roughness Reynolds Number.

    12

    u*eν

    11.6 /δν( )e = u*e /ν ≤ 3.5 Smooth flow3.5< 11.6 /δν( )e = u*e /ν < 70 Transition flow70 ≤ 11.6 /δν( )e = u*e /ν Wholly rough flow