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002a Unit Pressure

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Carmela Marie Lingad – Oliquino
MSCE – Geotechnical, SO2
Fluid Statics
Unit Pressure
TOPIC
OUTLINE
Pascal’s Law
Atmospheric, Absolute And Gage Pressure
Instruments
Pressure Variations
Pressure Head
TOPIC
OUTLINE
Piezometer
Manometer
Fluid Statics
Unit Pressure
TOPIC
OUTLINE
Pascal’s Law
Atmospheric, Absolute And Gage Pressure
Instruments
Fluid Statics
• Study of pressures throughout a fluid at rest and the pressure forces on finite
surfaces.
• Pressure at any point P on a plane surface.
• The limiting value of the ratio of normal force to surface area as the area
approaches zero size.
• Newtons per square meter (Pascals, Pa) or in bars (1 bar = 105 N/m2 or 105 Pa)
Fluid Statics
Unit Pressure
TOPIC
OUTLINE
Pascal’s Law
Atmospheric, Absolute And Gage Pressure
Instruments
Unit Pressure Or Pressure, P
• Pressure is the force per unit area exerted by a liquid or gas on a body or surface,
with the force acting at right angles to the surface uniformity in all directions.
• The intensity of pressure (known also as unit pressure or simply called pressure)
is the amount of force exerted by a fluid distributed uniformly over a unit area
Equation for Unit Pressure Or
Pressure, P
𝑭
𝑷=
𝑨
where: P – pressure in Pascal (Pa)
F – force in Newton (N)
A – area in square meter (m2)
Equation for Unit Pressure Or
Pressure, P
• If the unit pressure is not uniform over
the unit area, it can be expressed as the
sum of differential pressure.
𝒃
𝒅𝑭
𝒑=ΰΆ±
𝒂 𝒅𝑨
Unit Pressure Or Pressure, P
• Since fluid at rest cannot resist shearing stress, pressure is always at right angle
to the area where it is acting. It is also worthy to note that the total hydrostatic
force F = pA, which can be found by cross multiplication.
• Units:
pounds per square inch (psi)
kg/cm2 or atmosphere (atm)
N/m2 (Pascal, Pa)
English system
International usage
Metric system
Fluid Statics
Unit Pressure
TOPIC
OUTLINE
Pascal’s Law
Atmospheric, Absolute And Gage Pressure
Instruments
Pascal’s Law
• Developed by French mathematician, Blaise Pascal
• Pascal's law states that the pressure at a point in a fluid at rest is the same in all
directions.
• This means it is independent of the orientation of the surface around the point.
Pascal’s Law
• Consider a small triangular prism of unit length
surrounding the point in a fluid at rest.
Pascal’s Law
• Since the body is in static equilibrium, we can write
𝑃1 : 𝐴𝐡 × π‘™ − 𝑃3 𝐡𝐢 × π‘™ cos πœƒ = 0 (π‘’π‘ž. 𝑖)
𝑃2 : 𝐴𝐡 × π‘™ − 𝑃3 𝐡𝐢 × π‘™ sin πœƒ − π‘Š = 0 (π‘’π‘ž. 𝑖𝑖)
• From Equation (i) 𝑃1 = 𝑃3 since cos πœƒ = 𝐴𝐡𝐡𝐢, and
Equation (ii) gives 𝑃2 = 𝑃3 since sin πœƒ = 𝐴𝐢𝐡𝐢,and π‘Š =
0 as the prism shrinks to a point.
𝑃1 → 𝑃2 → 𝑃3
Pascal’s Law
• Consider an elementary cylindrical volume of fluid (of
length, L and cross-sectional area, dA) within the static
fluid mass (Figures 2.2), p being the pressure at an
elevation of y and dp being the pressure variation
corresponding to an elevation variation of dy.
• For equilibrium of the elementary volume,
𝑝𝑑𝐴 − πœŒπ‘”π‘‘π΄πΏ sin πœƒ − 𝑝 + 𝑑𝑝 𝑑𝐴 = 0
Or
𝑑𝑝 = − πœŒπ‘”π‘‘π‘¦
since
𝑑𝑦
sin πœƒ =
𝐿
Pascal’s Law
• The laws of fluid mechanics are observable in
many everyday situations. For example, the
pressure exerted by water at the bottom of a
pond will be the same as the pressure exerted
by water at the bottom of a much narrower
pipe provided depth remains constant.
Fluid Statics
Unit Pressure
TOPIC
OUTLINE
Pascal’s Law
Atmospheric, Absolute And Gage Pressure
Instruments
Atmospheric Pressure, Patm
• It is the weight of all gases above the surface in which it comes in contact.
• Under normal conditions at sea level
1 atm = 1.03323 kg/cm2
= 14.696 psi
= 760 mm Hg
= 29.921 in Hg
= 101,325.024 Pa
= 760 Torr
= 1.01325 bar
Gage Pressure (Relative Pressure)
• Gage Pressure are pressures above or below the atmosphere and can be
measured by pressure gauges or manometers.
• Negative gauge pressure indicates a vacuum which cannot go below –101.325 kPa.
• Positive gauge pressure indicates that the pressure is above atmospheric.
π‘·π’ˆπ’‚π’ˆπ’† = πœΈπ’‰
Absolute Pressure
• Absolute pressure (pabs) is equal to gauge pressure plus atmospheric pressure.
There is no such thing as negative absolute pressure. In the absence of all matter
(complete vacuum), the absolute pressure is zero.
𝑷𝒂𝒃𝒔 = π‘·π’ˆπ’‚π’ˆπ’† + π‘·π’‚π’•π’Ž
• Note: The term pressure, unless otherwise specified, will be used to denote gage
or relative pressure.
Fluid Statics
Unit Pressure
TOPIC
OUTLINE
Pascal’s Law
Atmospheric, Absolute And Gage Pressure
Instruments
Gage Pressure (Relative Pressure) –
Bourdon Gauge
• For a higher pressure differences, a Bourdon
gauge, named after the French inventor
Eugene Bourdon, is used.
• This consists of a hollow metal tube with an
oval cross section, bent in the shape of a
hook. One end of the tube is closed, the other
open and connected to the measurement
region.
Gage Pressure (Relative Pressure) –
U-Tube Manometer
• For small pressure differences, a U-Tube
manometer is used.
• It consists of a U-shaped tube with one end
connected to the container and the other
open to the atmosphere.
• Filled with a liquid, such as water, oil, or
mercury, the difference in the liquid surface
levels in the two manometer legs indicates
the pressure differences from local
atmospheric conditions.
Absolute Pressure – Barograph
• a recording barometer which provides a
continuous record of pressure over a period of
time
Absolute Pressure – Aneroid Barometer
• In an aneroid barometer, a partially
evacuated metal drum expands or contracts
in response to changes in air pressure. A
series of levers and springs translates the up
and down movement of the drum top into the
circular motion of the pointers along the
aneroid barometer’s face.
Absolute Pressure – Mercury Barometer
• A mercury barometer is an accurate and
relatively simple way to measure changes in
atmospheric pressure.
• At sea level, the weight of the atmosphere
forces mercury 760mm (29.9 in) up a
calibrated glass tube.
• Higher elevations yield lower readings
because the atmosphere is less dense there,
and the thinner air exerts less pressure on the
mercury.
Pressure Variations
Pressure Head
TOPIC
OUTLINE
Piezometer
Manometer
Variations on Pressure
• The difference in pressure between
any two points in a homogenous fluid
at rest is equal to the product of the
unit weight of the fluid (𝛾) to the
vertical distance h) between the
points.
Variations on Pressure
π‘·πŸ = π‘·πŸ + πœΈπ’‰
• Any change in pressure at point 1 would
cause an equal change to the pressure
in point 2.
• A pressure applied at any point in a
liquid at rest is transmitted equally and
undiminished to every point in the
liquid.
Variations on Pressure
• Assume the point 1 lies on the free
liquid surface, then the gauge pressure
at point 1 is zero and the equation
becomes:
𝑷 = πœΈπ’‰
• The pressure at any point “h” below a
free liquid surface is equal to the
product of the unit weight of the fluid
and the height.
Variations on Pressure
• Assume the points 1 and 2 lie on the
same elevation, such that h = 0; then
the equation becomes:
π‘·πŸ = π‘·πŸ
• The pressure along the same horizontal
plane in a homogenous fluid at rest is
equal.
Pressure Variations
Pressure Head
TOPIC
OUTLINE
Piezometer
Manometer
Pressure Head
• The equation P = γh may be written into the form
𝑷
𝒉=
𝜸
• where h or its equivalent P/γ is in hydraulics called the pressure head. Pressure
head is the height of column of homogeneous fluid of unit weight γ that will
produce an intensity of pressure P.
To convert pressure head of liquid A to equivalent pressure head of
liquid B
𝒔𝑨
𝝆𝑨
πœΈπ‘¨
𝒉𝑩 =
𝒉𝑨 =
𝒉𝑨 =
𝒉𝑨
𝒔𝑩
𝝆𝑩
πœΈπ‘©
To convert pressure head of any liquid to equivalent pressure head
of water
π’‰π’˜π’‚π’•π’†π’“ = π’”π’π’Šπ’’π’–π’Šπ’… × π’‰π’π’Šπ’’π’–π’Šπ’…
where: s = specific gravity
𝛾 = unit weight
𝜌 = density
Pressure Variations
Pressure Head
TOPIC
OUTLINE
Piezometer
Manometer
Piezometer
• Piezometer is the simplest form of manometer which is tapped into the wall of
pressure conduit for the purpose of measuring pressure.
• Though effective in many purposes, piezometer is not practical to use in lighter
liquids with large pressure and cannot be used to measure gas pressure.
Piezometer
• From the figure, three piezometers A, B,
and C are attached to a pressure conduit at
bottom, top, and side, respectively.
• The column of liquid at A, B, and C will rise
at the same level above M indicating a
positive pressure at M.
• Also, the piezometer D measures the
negative pressure at N.
Pressure Variations
Pressure Head
TOPIC
OUTLINE
Piezometer
Manometer
Manometer
• Manometer is a simple and inexpensive device of measuring pressure and
pressure difference. It is usually bent to form a U-tube and filled with liquid of
known specific gravity. The surface of the liquid will move in proportion to
changes of pressure.
Open Manometer
• Open manometer is a tube bent into a Ushape to contain one or more fluids of
different specific gravities. It is used to
measure pressure.
Differential Manometer
• Differential manometer cannot measure
pressure but can measure pressure
difference. Frequently in hydraulic
problems, difference in pressure is more
useful information than the pressure itself.
Draw a sketch of the
manometer system
approximately to scale.
Number in order all levels of
contact of the different
fluids, starting with level 0
at the free surface.
Decide on the fluid of which
head are to be expressed.
Water is more desirable. In
most cases, we suggest to
use head in water even if
there is no water in the
system
Starting from level 0 (zero
gage pressure) at free
surface, proceed from level
to level adding or
subtracting as the elevation
increases or decreases giving
due regard to the specific
gravity of the fluid.
Carmela Marie Lingad – Oliquino
MSCE – Geotechnical, SO2
β–ͺ A tank contains oil of SG = 0.80, gasoline of SG = 0.90 and seawater of SG = 1.03. If
the depth of the liquids are 0.50 m, 0.80 m and 1 m for the oil, gasoline and
seawater respectively.
a. Find the pressure at a depth of 1.20m. (Ans. 10.10 kPa)
b. Find the pressure at a depth of 1.8m. (Ans. 16.04 kPa)
c. Find the pressure at the bottom of the tank. (Ans. 21.09 kPa)
β–ͺ If the pressure at a point in the ocean is 60 kPa, what is the pressure 27 m below
this point?
𝑃2 = 𝑃1 + π›Ύβ„Ž
𝑃2 = 60 π‘˜π‘ƒπ‘Ž + 9.81 π‘˜π‘ΰ΅— 3 1.03 27 π‘š
π‘š
𝑷 = πŸ‘πŸ‘πŸ. πŸ–πŸ π’Œπ‘·π’‚
β–ͺ If the pressure in the air space above an oil (SG = 0.75) surface in a closed tank is
115 kPa absolute, what is the gage pressure 2 m below the surface?
π‘ƒπ‘Žπ‘‘π‘š = 101.325 π‘˜π‘ƒπ‘Ž
𝑃 = π‘ƒπ‘ π‘’π‘Ÿπ‘“π‘Žπ‘π‘’ + π›Ύβ„Ž
π‘ƒπ‘ π‘’π‘Ÿπ‘“π‘Žπ‘π‘’ = 115 π‘˜π‘ƒπ‘Ž − 101.325 π‘˜π‘ƒπ‘Ž
π‘ƒπ‘ π‘’π‘Ÿπ‘“π‘Žπ‘π‘’ = 13.675 π‘˜π‘ƒπ‘Ž
𝑃 = 13.675 π‘˜π‘ƒπ‘Ž + 9.81 π‘˜π‘ΰ΅— 3
π‘š
𝑷 = πŸπŸ–. πŸ‘πŸ— π’Œπ‘·π’‚
2π‘š
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