Water flow in pipes Flashcards

1
Q

Define the type of pressure pipe flow we study in this class

A

refers to full water flow in closed conduits of circular cross section under s certain pressure gradient

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

What are the 4 factors the describe pipe flow

A

Cross section
elevation
pressure
mean velocity

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

how do we find the mean velocity (equation)

A

V = Q/A

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

what is the equation for the cross section of a pipe

A

A = π/4 D^2

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

What did Reynold determine was the affecting factors to turn laminar flow into turbulent flow

A

velocity, pipe diameter, and the kinematic viscosity
Re = NR =𝜌VD/u = VD/v
where V is mean velocity
v is kinematic viscosity = u/𝜌

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

For a circular pipe, what is the range of NR for laminar flow

A

NR <= 2000

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

What is the special way to find the mean velocity in laminar flow

A

V = Vmax/2
Where Vmax is the center line of velocity in the pipe

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

For a circular pipe, what is the range of NR for transitional flow

A

2000 < NR < 4000
also called the critical zone

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

For a circular pipe, what is the range of NR for turbulent flow

A

> = 4000

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Describe figure 3.2 in the book 2. How does laminar flow vs. turbulent floe look like in pipes?

A

Laminar: parabolic distribution where the mean velocity is equal to one half times the max center line velocity
Turbulent: Logarithmic distribution, as NR gets larger, the center velocity distribution gets flatter.
We can also say that turbulent velocity distribution is more uniform than laminar distribution near the center of the pipe

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Under ordinary circumstances, water loses energy as it flows through the pipes. This is caused by

A

1) friction against the pipe walls
2) viscous dissipation occurring throughout the flow

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

What does wall friction depend on

A

roughness of the wall material (e) and the shear rate/velocity gradient dv/dr at the wall

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

Higher fiction loss may be expected as the Reynolds number ____________

A

increases

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Describe what viscous dissipation is

A

momentum transfer of water molecules between layers is intensified as the flow becomes more turbulent.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

rate of energy loss in pipe flow varies as a function of

A

Reynolds number and the roughness of the pipe wall

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

What is the equation for continuity in pipe flows

A

A1V1 = A2V2 = Q = constant

17
Q

how do we derive the equation for continuity in pipe flows

A

1)mass flow rate into CV =𝜌1V1A1
2) mass flow rate out CV = 𝜌2V2A2
3) Net mass flow rate 𝜌1V1A1 = 𝜌2V2A2 (conservation law of mass)
4) for steady incompressible flow the rate of change is 0: 𝜌1V1A1 - 𝜌2V2A2 = 0
5) 𝜌1 - 𝜌2 constant
6) A1V1 = A2V2 = Q = constant

18
Q

What is the momentum equation in pipe flow

A

∑𝑭 ⃑ = 𝝆𝑸(𝑽𝟐 ⃑ −𝑽𝟏 ⃑ )

19
Q

What is the momentum equation in pipe flow in scalar form in the x-direction

A

∑𝑭x ⃑ = 𝝆𝑸(𝑽x𝟐 ⃑ −𝑽x𝟏 ⃑ )

20
Q

What are the 3 basics forms that energy appears from water flowing in pipes

A
  1. Potential energy related to the elevation (h)
  2. kinetic energy related to the motion (V)
  3. Pressure energy related to the Pressure (P)
21
Q

How can we express the potential energy equation in pipe flow

A

𝝆A1V1gh1 - 𝝆A2V2gh2
where m = 𝝆Q
and 𝝆Qgh = 𝝆AVgh

22
Q

How can we express the kinetic energy equation in pipe flows

A

mV^2 /2
𝝆QV^2 /2
𝝆A1V1(V1^2 /2) - 𝝆A2V2(V2^2 / 2)

23
Q

How can we express the pressure energy equation in pipe flow

A

hydrostatic force - pressure force opposing the flow
P1A1V1 - P2A2V2

24
Q

Using all the energy equations, how do we derive the overall energy equation

A

(ρA1V1gh1−ρA2V2gh2)+(ρA1V1(V1^2)/2 −ρA2V2 (V2^2)/2 )+(𝑃1𝐴1𝑉1−𝑃2𝐴2𝑉2)

Divide by ρgQ, Q = AV and γ=ρg we get

ℎ1+𝑃1/γ+𝑉1^2/2𝑔=ℎ2+𝑃2/γ
+𝑉2^2/2g

25
The sum of _____________, ________________, and the _______________ accounts for 3 different energies contained in a unit weight of water flowing through a particular section of pipe or CV between section
the elevation head, the pressure head, and the velocity head
26
describe the head loss
during the flow between upstream and downstream sections, a certain amount of hydraulic energy is lost because of friction
27
describe how the energy equation changes when we consider head loss
H1 = upstream and H2 = downstream H1 > H2 H1 = H2 + hL
28
What is hL when we have a horizontal pipe of uniform size
hL = (P1 - P2) / y
29
what is hL when we have a uniform size pipe
(P1 - P2) /y = hL +h2-h1
30
what is friction head loss
friction loss in flow is a lot more significant than viscous dissipation. therefore the head loss is equal to the friction head loss. hL = hf
31
what is the equation for the friction head loss
hf = f(L/D) (Vavg^2 / 2g)
32
When we have turbulent flow, the friction factor depends less on _________ and ___________ dominates
Reynolds number (NR) relative roughness(e/D)
33
what are the 4 zones of pipe flow in the moody diagram of friction factors for pipe
1) laminar where ln(f) is a linear function of NR 2) A critical zone where f is uncertain because flow is neither laminar or turbulent 3) a transitional zone where f is a function of NR and e/D 4) turbulent flow where f depends on e/D and is independent of NR
34
How do we find the friction factor f
We find the roughness of the material e in table 3.1 book 2, then get relative roughness e/D Once Nr is also known we can use figure 3.8 to find f of circular pipes