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Fluid Mechanics

Fluid Mechanics

FFlluiuid Mechd Mechananiics cs

Chapter 6 Equation Momentum Equation: Derivation (Read Chapter 6 and Section 7.6).6)

1 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø For the analysis of and moments produced by flowing fluids Ø RTT is applied to Newton’ s 2nd law of motion (F=ma) Ø Develop the Eulerian form of the momentum equation

2 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø Principle: The rate of change of momentum of a body is equal to the acting on the body Ø Newton’ s second law of motion: ΣF = mm a

l where FF and a

l and is constant Ø Writing this in terms of momentum for a single particle… …

3 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø Writing this in terms of momentum for a group of particles (like a fluid system)m) …

l where Mom sys id the total momentum of all mass comprising the system

l This is the Lagrangian equation

4 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø Now use RTT to derive the Eulerian eqn.

l where B sys = Mom sys l and b = vector velocity (v)

l Note: velocity must be relative to an inertial reference frame (does not rotate) and can be either stationary or moving at a constant velocity..

5 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø Now use RTT to derive the Eulerian eqn.

Ø Substitute B sys and b… …

6 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø Combining...

Ø Yields the integral form of the momentum equation… …

7 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø Integral form of the momentum equation…

Ø Can be expressed in words as

Ø Note: the momentum equation is a vector equation (i.e. there is direction associated with it)

8 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø If velocity is uniformly distributed across each port, then…

Ø becomes...

l where “o o ” refers to outlet and “i i ” refers to inlet

l Note that ṁṁ v has the same units as F and is the momentum per time

l Applies to any cv including one that is moving, deforming or bothh

9 MomenMomenttumum EqEquauattionion:: DDererivivaattionion

Ø The three components of…

Ø in cartesian coordinates are...

10 FFlluiuid Mechd Mechananiics cs

Chapter 6 Momentum Equation Momentum Equation: Interpretation (Read Chapter 6 and Section 7.6).6)

11 ForForcce e TerTermsms

Ø Terminology

l Force diagramm : shows the forces acting on the matter contained within a control volume. • A force diagram is equivalent to a free­ b ody diagram at the instant in time when the momentum equation is applied.

l Body force: A force that acts on mass elements within the body is defined ()

l Surface forcerce : as a force that requires physical contact, meaning that surface forces act at the control surface ( ( pAA )

12 ForForcce e TerTermsms

Ø Consider the force diagrams (FD) in (b) and (c) Ø What are the forces acting on the pipe of D diameter and L length?

13 ForForcce e TerTermsms

Ø Figure (b): cv inside the pipe

14 ForForcce e TerTermsms

Ø Figure (c): cv outside the pipe

15 ForForcce e TerTermsms

Ø Choice of cv is dependent on what you want to know. Ø (b) to relate the pressure change between 1 & 2 to wall shear stress Ø (c) to calculate tensile force carried by pipee

16 MomenMomenttumum AAccccumuumulatilationon

Ø The momentum accumulation term is the first term on the right side of = sign

Ø It is the momentum of the material inside the control volume Ø Many problem it equals zero if

l Steady flow through a control volume and

l Stationary structure and

l Constant density

17 MomenMomenttumum DDiiagagraram m

Ø Momentum diagramm : created by sketching a control volume and then drawing a vector to represent the momentum accumulation term and a vector to represent momentum flow at each section where mass crosses the control surface

18 MomenMomenttumum DDiiagagraram m

Ø Consider the moment diagram beloww …

Ø And assume that the velocity is constant. Ø Therefore, the momentum accumulation term = 0

19 MomenMomenttumum DDiiagagraram m

Ø Outlet momentum flow is

Ø Inlet momentum flow iss

20 MomenMomenttumum DDiiagagraram m

Ø Therefore, net outward flow of momentum iss ……

21 IInn ­­ cclalassss ExaExammpleple ProbProblelem m

Ø A horizontal circular jet of water at 15 0 C is discharged from a tank and then strikes a vertical plate. Ø The axis of the jet is normal to the plate Ø The cross­ s ectional area of the jet is 0.015m 2 . Ø What velocity in the jet is needed to produce a force of 2000N on the plate? Ø What pressure at A in the tank is needed to produce this velocity??

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