Displacement Thickness
&
Momentum Thickness
1
Group Members
GC Jabran Naveed
Cheema
GC Haroon ur Rashid
GC Bilal Masood
NS Ashir Azeem
A boundary layer is the layer of fluid in the immediate vicinity of a bounding
surface where the effects of viscosity are significant.
Boundary
Layers
2
3
There are three main definitions of boundary layers :
1. Boundary layer thickness
2. Displacement thickness
3. Momentum thickness
Boundary layer equations represent a significant simplification over the full Navier-Stokes
equations in a boundary layer region.
For simplicity, we determine equations for steady, incompressible, uniform flow over a flat
plate. The equations for flow over curved surfaces, and for non-uniform flow, differ only
slightly. The equations for compressible boundary layers are somewhat more complex than
the incompressible equations; we will not consider them here.
4
Assumptions
The boundary layer equations require several assumptions about the flow in the boundary layer.
1. All of the viscous effects of the flow field are confined to the boundary layer, adjacent to the wall .
Outside of the boundary layer, viscous effects are not important, so that flow can be determined by in viscid
solutions such as potential flow or Euler equations.
2.The viscous layer is thin compared to the wall.
3.The boundary conditions of the boundary layer region are the no-slip condition at the wall, and the free-
stream condition at infinity:
 δ(x) is the boundary layer thickness when u(y) =0.99V
 V is the free-stream velocity
 The purpose of the boundary layer is to allow the fluid to change its
velocity from the upstream value of V to zero on the surface
5Boundary Layer Thickness
 There is a reduction in the flow
rate due to the presence of the
boundary layer
 This is equivalent to having a
theoretical boundary layer with
zero flow
Displacement Thickness 6
Mathematically
:
Because of the velocity deficit, within the boundary layer, the flow rate across
section b–b is less than that across section a–a. However, if we displace the plate at
section a–a by an appropriate amount the boundary layer displacement thickness,
the flow rates across each section will be identical.
7
Where b is plate width
Momentum Thickness 8
 Momentum thickness is a measure of the boundary layer thickness.
 It is defined as the distance by which the boundary should be displaced to
compensate for the reduction in momentum of the flowing fluid on account of
boundary layer formation
 The momentum thickness, symbolized by Ө is the distance that, when multiplied by the
square of the free-stream velocity, equals the integral of the momentum defect, across the
boundary layer.
9
It is often used when determining the drag on an object. Again because of the
velocity deficit U-u, in the boundary layer, the momentum flux across section b–b in
Fig. 9.8 is less than that across section a–a. This deficit in momentum flux for the
actual boundary layer flow on a plate of width b is given by
Mathematically
:
which by definition is the momentum flux in a layer of uniform speed U and thickness
Ө.That is,
10
Thank You
11

Boundary Layer Displacement Thickness & Momentum Thickness

  • 1.
    Displacement Thickness & Momentum Thickness 1 GroupMembers GC Jabran Naveed Cheema GC Haroon ur Rashid GC Bilal Masood NS Ashir Azeem
  • 2.
    A boundary layeris the layer of fluid in the immediate vicinity of a bounding surface where the effects of viscosity are significant. Boundary Layers 2
  • 3.
    3 There are threemain definitions of boundary layers : 1. Boundary layer thickness 2. Displacement thickness 3. Momentum thickness Boundary layer equations represent a significant simplification over the full Navier-Stokes equations in a boundary layer region. For simplicity, we determine equations for steady, incompressible, uniform flow over a flat plate. The equations for flow over curved surfaces, and for non-uniform flow, differ only slightly. The equations for compressible boundary layers are somewhat more complex than the incompressible equations; we will not consider them here.
  • 4.
    4 Assumptions The boundary layerequations require several assumptions about the flow in the boundary layer. 1. All of the viscous effects of the flow field are confined to the boundary layer, adjacent to the wall . Outside of the boundary layer, viscous effects are not important, so that flow can be determined by in viscid solutions such as potential flow or Euler equations. 2.The viscous layer is thin compared to the wall. 3.The boundary conditions of the boundary layer region are the no-slip condition at the wall, and the free- stream condition at infinity:
  • 5.
     δ(x) isthe boundary layer thickness when u(y) =0.99V  V is the free-stream velocity  The purpose of the boundary layer is to allow the fluid to change its velocity from the upstream value of V to zero on the surface 5Boundary Layer Thickness
  • 6.
     There isa reduction in the flow rate due to the presence of the boundary layer  This is equivalent to having a theoretical boundary layer with zero flow Displacement Thickness 6
  • 7.
    Mathematically : Because of thevelocity deficit, within the boundary layer, the flow rate across section b–b is less than that across section a–a. However, if we displace the plate at section a–a by an appropriate amount the boundary layer displacement thickness, the flow rates across each section will be identical. 7 Where b is plate width
  • 8.
    Momentum Thickness 8 Momentum thickness is a measure of the boundary layer thickness.  It is defined as the distance by which the boundary should be displaced to compensate for the reduction in momentum of the flowing fluid on account of boundary layer formation  The momentum thickness, symbolized by Ө is the distance that, when multiplied by the square of the free-stream velocity, equals the integral of the momentum defect, across the boundary layer.
  • 9.
    9 It is oftenused when determining the drag on an object. Again because of the velocity deficit U-u, in the boundary layer, the momentum flux across section b–b in Fig. 9.8 is less than that across section a–a. This deficit in momentum flux for the actual boundary layer flow on a plate of width b is given by
  • 10.
    Mathematically : which by definitionis the momentum flux in a layer of uniform speed U and thickness Ө.That is, 10
  • 11.