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St Venant Equations Reading: Sections 9.1 – 9.2

St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

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Page 1: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

St Venant Equations

Reading: Sections 9.1 – 9.2

Page 2: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

2

Types of flow routing

• Lumped/hydrologic– Flow is calculated as a function of time alone at a

particular location– Governed by continuity equation and

flow/storage relationship • Distributed/hydraulic

– Flow is calculated as a function of space and time throughout the system

– Governed by continuity and momentum equations

Page 3: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular
Page 4: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular
Page 5: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Distributed Flow routing in channels

• Distributed Routing• St. Venant equations

– Continuity equation

– Momentum Equation

0

t

A

x

Q

What are all these terms, and where are they coming from?

0)(11 2

fo SSgx

yg

A

Q

xAt

Q

A

Page 6: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Assumptions for St. Venant Equations

• Flow is one-dimensional• Hydrostatic pressure prevails and vertical

accelerations are negligible• Streamline curvature is small. • Bottom slope of the channel is small.• Manning’s equation is used to describe

resistance effects• The fluid is incompressible

Page 7: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Continuity Equation

dxx

QQ

x

Q

t

Adx

)(

Q = inflow to the control volume

q = lateral inflow

Elevation View

Plan View

Rate of change of flow with distance

Outflow from the C.V.

Change in mass

Reynolds transport theorem

....

.0scvc

dAVddt

d

Page 8: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Continuity Equation (2)

0

t

A

x

Q

0)(

t

y

x

Vy

0

t

y

x

Vy

x

yV

Conservation form

Non-conservation form (velocity is dependent variable)

Page 9: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Momentum Equation

• From Newton’s 2nd Law: • Net force = time rate of change of momentum

....

.scvc

dAVVdVdt

dF

Sum of forces on the C.V.

Momentum stored within the C.V

Momentum flow across the C. S.

Page 10: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Forces acting on the C.V.

Elevation View

Plan View

• Fg = Gravity force due to weight of water in the C.V.

• Ff = friction force due to shear stress along the bottom and sides of the C.V.

• Fe = contraction/expansion force due to abrupt changes in the channel cross-section

• Fw = wind shear force due to frictional resistance of wind at the water surface

• Fp = unbalanced pressure forces due to hydrostatic forces on the left and right hand side of the C.V. and pressure force exerted by banks

Page 11: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Momentum Equation

....

.scvc

dAVVdVdt

dF

Sum of forces on the C.V.

Momentum stored within the C.V

Momentum flow across the C. S.

0)(11 2

fo SSgx

yg

A

Q

xAt

Q

A

Page 12: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

0)(

fo SSgx

yg

x

VV

t

V

0)(11 2

fo SSgx

yg

A

Q

xAt

Q

A

Momentum Equation(2)

Local acceleration term

Convective acceleration term

Pressure force term

Gravity force term

Friction force term

Kinematic Wave

Diffusion Wave

Dynamic Wave

Page 13: St Venant Equations Reading: Sections 9.1 – 9.2. 2 Types of flow routing Lumped/hydrologic – Flow is calculated as a function of time alone at a particular

Momentum Equation (3)

fo SSx

y

x

V

g

V

t

V

g

1

Steady, uniform flow

Steady, non-uniform flow

Unsteady, non-uniform flow