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Monroe L. Weber-Shir k S chool of Civil and Environmental Engi neering Statics CEE 331 March 25, 2022
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Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Dec 19, 2015

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Page 1: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Monroe L. Weber-Shirk

School of Civil and

Environmental Engineering

StaticsStaticsCEE 331

April 18, 2023

Page 2: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Definitions and Applications

Statics: no relative motion between adjacent fluid layers.Shear stress is zeroOnly _______ can be acting on fluid surfaces

Gravity force acts on the fluid (____ force)Applications:

Pressure variation within a reservoir Forces on submerged surfacesTensile stress on pipe wallsBuoyant forces

pressure

body

Page 3: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Motivation?What are the pressure

forces behind the Hoover Dam?

Page 4: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Upstream face of Hoover Dam

Upstream face of Hoover Dam in 1935

Crest thickness: 13.7 m Base thickness: 201 mWHY???

Page 5: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

What do you think?

Lake Mead, the lake behind Hoover Dam, is the world's largest artificial body of water by volume (35 km3). Is the pressure at the base of Hoover Dam affected by the volume of water in Lake Mead?

Page 6: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

What do we need to know?

Pressure variation with directionPressure variation with locationHow can we calculate the total force on a

submerged surface?

Page 7: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure Variation with Direction(Pascal’s law)

yy

xx

pss

pxy

pyx

y

x

s

2

g x y

Body forces

Surface forcesEquation of Motion

xF

F = ma

02

m xx ayx

a

y sin s

0y p -y p sx

pxy - pss sin

Pressure is independent of direction!

Page 8: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure Field (pressure variation with location)

In the absence of shearing forces (no relative motion between fluid particles) what causes pressure variation within a fluid?

Consider a soda can in space…Throw the soda can to another astronaut…Throw the soda can toward the moon

What causes pressure gradients?

Page 9: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

p

pz

zx y

FH IK 2

Pressure Field

ppy

yx z

FHG

IKJ

2

m x y zji

zz

yy

xx

k

ppz

zx y

FH IK 2

ppy

yx z

FHG

IKJ

2

Small element of fluid in pressure gradient with arbitrary __________.

Forces acting on surfaces of elementPressure is p at

center of element

acceleration

Mass…Mass…

Same in x!Same in x!Now let’s sum the forces in the y direction

Page 10: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Simplify the expression for the force acting on the element

Fpy

x y zy

Fpx

x y zx

Fpz

x y zz

F i j k

FHG

IKJ

px

py

pz

x y z

px

py

pz

p i j k

F p x y z

Same in xyz!

This begs for vector notation!

Forces acting on element of fluid due to pressure gradient

2 2y

p y p yF p x z p x z

y y

Page 11: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Apply Newton’s Second Law

F a m

p x y z x y z a

p a

F p x y z

m x y za ad rd d d= Mass of element of fluid

Substitute into Newton’s 2nd Law

Obtain a general vector expression relating pressure gradient to acceleration and write the 3 component equations.

We are effectively accelerating upward at g when we are “at rest” on earth’s surface!

x y z

p p pa a a

x y zr r r

¶ ¶ ¶= =- -

¶=-

¶ ¶

dpdz

g

ˆp r g- Ñ = +a k Text version of eq.

At rest

3 component equations

Pressure in direction of a.

A surface of constant pressure?

Page 12: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Changing density

Changing gravity

Pressure Variation When the Specific Weight is Constant

What are the two things that could make specific weight () vary in a fluid?

= g

Piezometric head is constant in a static incompressible fluid

dp dz

dp dzp

p

z

z

1

2

1

2z z

p p z z2 1 2 1 a f pz

pz1

12

2

Constant specific weight!

Generalize to any a!

Page 13: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

p hgD =

Example: Pressure at the bottom of a Tank of Water?

Does the pressure at the bottom of the tank increase if the diameter of the tank increases? h

1

2

p p z z2 1 2 1 a f

What is the pressure at the top of the tank?

Suppose I define pressure and elevation as zero at the water surface. What is the piezometric head everywhere in the tank?

Zero!

No! ?p

zg+ =

z Free surface

11

pz

Page 14: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

6894.76 Pa/psi

Units and Scales of Pressure Measurement

Standard atmospheric pressure

Local atmospheric pressure

Absolute zero (complete vacuum)

Absolute pressureGage pressure

1 atmosphere101.325 kPa14.7 psi______ m H20760 mm Hg

Suction vacuum(gage pressure)Local baromet

er reading10.34

atmph

g= =

3

3

101 109806 /

x PaN m

Page 15: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Mercury Barometer (team work)

22

11 z

p z

p

6.13HgSWhat is the local atmospheric pressure (in kPa) when R is 750 mm Hg?

R

1

2

1221 zzp p Hg P2 = Hg vapor pressure

R p Hg1

waterHgHg S

RS p Hg1

PammN p 000,10075.0/98066.13 31

Hg

water

r

r=

Assume constant

Page 16: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure Variation in a Compressible Fluid

Perfect gas at constant temperature (Isothermal)

Perfect gas with constant temperature gradient

Page 17: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Perfect Gas at Constant Temperature (Isothermal)

p nRT gaspM

RT

g

dzRT

gpMdp gas

dzRT

gM

pdp

z

z

gasp

p

2

1

2

1

121

2ln zzRT

gM

pp gas

e

zzRT

gM gas

pp

12

12

Mgas is molecular mass

is function of pdp dz

gasnM

Integrate…

Page 18: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

= 0.00650 K/m

Perfect Gas with Constant Temperature Gradient

The atmosphere can be modeled as having a constant temperature gradient

zTT a

dzRT

gM

pdp gas

dzzTR

gM

pdp

a

gas

z

a

gasp

p zTdz

R

gM

pdp

a 0

a

agas

a TzT

R

gM

pp

ln

1ln 1

gasM g

R

aa

zp p

T

0

20

40

60

80

100

0 5000 10000 15000Elevation (m)

Pre

ssur

e (k

Pa)

Lapse rate

Mt. Everest

8,850 m

1gas

R

M ga

a

T pz

p

Page 19: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure Measurement

BarometersManometers

StandardDifferential

Pressure Transducers

Measure atmospheric pressure

Pressure relative to atm.

Pressure difference between 2 pts.

Page 20: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

A

Standard Manometers

What is the pressure at A given h?

Pressure in water distribution systems commonly varies between 25 and 100 psi (175 to 700 kPa). How high would the water rise in a manometer connected to a pipe containing water at 500 kPa?

h

p = h

h = p/h = 500,000 Pa/(9800 N/m3)

h = 51 m Why is this a reasonable pressure?Why is this a reasonable pressure?

gage

Page 21: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

P1 = 0 h1

??

h2

Manometers for High Pressures

Find the gage pressure in the center of the sphere. The sphere contains fluid with 1 and the manometer contains fluid with 2.

What do you know? _____

Use statics to find other pressures.

1

2

3

=P3

1

2

For small h1 use fluid with high density. Mercury!

+ h12 - h21P1

Page 22: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

- h2Hg- h3w

Differential Manometers

h1

h3

Mercury

Find the drop in pressure between point 1 and point 2.

p1p2Water

h2

orifice

= p2

p1 - p2 = (h3-h1)w + h2Hg

p1 - p2 = h2(Hg - w)

p1 + h1w

Page 23: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Procedure to keep track of pressures

Start at a known point or at one end of the system and write the pressure there using an appropriate symbol

Add to this the change in pressure to the next meniscus (plus if the next meniscus is lower, and minus if higher)

Continue until the other end of the gage is reached and equate the expression to the pressure at that point

p1 + p = p2

Page 24: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure Transducers

Excitation: 10 Vdc regulated Output: 100 millivolts Accuracy: ±1% FS Proof Pressure: 140 kPa (20 psi) for 7 kPa model No Mercury! Can be monitored easily by computer Myriad of applications

Volume of liquid in a tank

Flow rates

Process monitoring and control

Full Scale

Page 25: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Types of Diaphragms Used for Pressure Measurements

Stainless SteelStrain gages bonded to the stainless steelTypical full scale output of 3 mV/V

PiezoresistiveStrain gage diffused into silicon wafersTypical full scale output of 10 mV/V

Page 26: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Silicon

Ideal material for receiving the applied force

Perfect crystalReturns to its initial shape (no hysteresis)Good elasticityNo need for special bonding between

material receiving force and strain gage

Page 27: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure Sensor Failure

High pressures – rupture crystal (beware of resulting leak!)

Water hammer – High speed pressure waves (speed of sound)Result from flow transients such as rapidly

shutting valvesInstall pressure snubber!

Incompatible materials

Elastic tubing or gas chamber

Page 28: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Absolute vs. Gage vs. Differential

AbsolutePort 2 sealed with vacuum

on bottom side of silicon crystal

GagePort 2 open to atmosphere

DifferentialBoth ports connected to

system

Port 1

Port 2

Page 29: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Pressure is independent of Pressure increases with

constant densitygas at constant temperaturegas with constant temperature gradient

Pressure scalesunitsdatum

Pressure measurement

direction

depthp = h

Use ideal gas law

Summary for Statics

dzdp

p a

Page 30: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Review

Pressure increases or decreases as we move in the direction of the acceleration vector?

The free surface is _______ to the acceleration vector.

What is an equation that describes the change in pressure with depth in a fluid?

Suppose a tank of fuel is accelerating upward at 2g. What is the change in pressure with depth in the fuel?

normal

dp adzr=-

pz

pz1

12

2

Page 31: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Statics example

What is the air pressure in the cave air pocket?

Page 32: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

Statics Lab

How did the bubbler work?How does the pressure sensor

read pressure at the bottom of the tank?

Must the pump be running if the water depth is decreasing?

Page 33: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Statics CEE 331 June 13, 2015

“Somebody finally got smart and came up with an above-ground pool that’s got a deep end and a shallow end.”