Assignment1_Solutions

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ENSC 388
Assignment #1 (Basic Concepts)
Assignment date: Wednesday Sept. 16, 2009
Due date: Wednesday Sept. 23, 2009
Problem 1: (Static Pressure)
Both a gage and a manometer are attached to a gas tank to measure its pressure. If
the reading on the pressure gage is 80 kPa, determine the distance between the two
fluid levels of the manometer if the fluid is (a) mercury (ρ =13,600 kg/m3) or (b)
water (ρ =1000 kg/m3).
Pg=80 kPa
GAS
h=?
Problem 2: (Buoyancy)
Balloons are often filled with helium gas because it weighs only about one-seventh
of what air weighs under identical conditions. The buoyancy force which can be
expressed as FB = ρairgVballoon will push the balloon upward. If the balloon has
diameter of 10 m and carries two people, 70 kg each, determine (a) the acceleration
of the balloon when it is first released and (b) the maximum amount of load, in kg,
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ENSC 388
Assignment # 1
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the balloon can carry. Assume the density of air is ρ =1.16 kg/m3, and neglect the
weight of the ropes and the cage. (Answers: 16.5 m/s2, 520.6 kg)
HELIUM
D=10 m
ρ=ρair/7
m=140 kg
Problem 3: (Hydrostatic pressure)
The lower half of a 10-m-high cylindrical container is filled with water (ρ =1000
kg/m3) and the upper half with oil that has a specific gravity of 0.85. Determine the
pressure difference between the top and bottom of the cylinder. (Answer: 90.7
kPa)
OIL
ρs=0.85
h=10 m
WATER
ρ =1000 kg/m3
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ENSC 388
Assignment # 1
2
Pg=80kPa
Patm
Problem 1:
2
Pg =80 kPa
Find h if:
h=?
GAS
3
a) Fluid is mercury (ρHg=13,600 kg/m )
b) Fluid is mercury (ρH2O=1000 kg/m3)
1
- Assumption:
The pressure is uniform in the tank, thus we can determine the pressure at the gage
port.
- Analysis
Starting with 𝑃𝑔 (gas pressure) and moving along the tube from point (1) by
adding (as we go down) or subtracting (as we go up), the ρgh term(s) until we
reach point (2), therefore;
𝑃𝑔 − πœŒπ‘”β„Ž = 𝑃2
Since tube at point (2) is open to atmosphere, 𝑃2 = π‘π‘Žπ‘‘π‘š .
𝑃𝑔 − 𝑃2 = πœŒπ‘”β„Ž
Pgage (What we read on the pressure gage)
π‘˜π‘”⁄
] × 9.81 [π‘š⁄ 2 ] β„Žπ»2 𝑂
π‘š3
𝑠
= 8.155[π‘š]
𝐻2 𝑂 → 80 × 103 [π‘ƒπ‘Ž] = 1000 [
⟹ β„Žπ»2 𝑂
80 kPa =ρgh
π‘˜π‘”⁄
] × 9.81 [π‘š⁄ 2 ] β„Žπ»π‘”
π‘š3
𝑠
= 0.599[π‘š]
𝐻𝑔 → 80 × 103 [π‘ƒπ‘Ž] = 13,600 [
⟹ β„Žπ»2 𝑂
{
FB
Problem 2:
D
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ENSC 388
Assignment # 1
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mhe
D=10 m
ρHe= ρair/7 and ρair =1.16 kg/m3
mpeople=140 kg
a
Assumption:
mpeople
The wight of the ropes and cage is neglected.
W
(Free body diagram)
Analysis:
Starting with free body diagram. We also know that te buoyancy force is:
𝐹𝐡 = πœŒπ‘Žπ‘–π‘Ÿ π‘”π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘›
π‘Š = π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ 𝑔
π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ = π‘šπ‘π‘’π‘œπ‘π‘™π‘’ + π‘šπ»π‘’
π‘šπ»π‘’ = πœŒπ»π‘’ π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘›
4 3
π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘› = πœ‹π‘…π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘›
3
4
π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘› = πœ‹(5[π‘š])3 = 523.59[π‘š3 ]
3
π‘šπ»π‘’ =
1
π‘˜π‘”
× 1.16 [ ⁄ 3 ] × 523.59[π‘š3 ] = 86.77
π‘š
7
π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ = π‘šπ»π‘’ + π‘šπ‘π‘’π‘œπ‘π‘™π‘’ = 86.77[π‘˜π‘”] + 140[π‘˜π‘”] = 226.77[π‘˜π‘”]
Newton law:
∑ 𝐹 = π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ × π‘Ž
Therefore:
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ENSC 388
Assignment # 1
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𝐹𝐡 − π‘Š = π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ × π‘Ž
(1)
πœŒπ‘Žπ‘–π‘Ÿ π‘”π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘› − π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ 𝑔 = π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™ π‘Ž
So,
π‘Ž=
πœŒπ‘Žπ‘–π‘Ÿ π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘› −π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™
π‘šπ‘‘π‘œπ‘‘π‘Žπ‘™
𝑔
(2)
Substituting values in Eq. (2),
π‘Ž=
1.16 [
π‘˜π‘”⁄
] × 523.59[π‘š3 ] − 226.77[π‘˜π‘”]
π‘š3
× 9.81 [π‘š⁄ 2 ]
𝑠
226.77[π‘˜π‘”]
π‘Ž = 16.46 [π‘š⁄ 2 ]
𝑠
The maximum amount of load that the balloon can carry can be calculated from;
∑𝐹 = 0
Using Eq. (1),
𝐹𝐡 = π‘Š
πœŒπ‘Žπ‘–π‘Ÿ π‘”π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘› = π‘šπ‘šπ‘Žπ‘₯ 𝑔
π‘šπ‘šπ‘Žπ‘₯ = πœŒπ‘Žπ‘–π‘Ÿ π‘‰π‘π‘Žπ‘™π‘™π‘œπ‘œπ‘› = 1.16 [
π‘˜π‘”⁄
] × 523.59[π‘š3 ] = 607.304
π‘š3
This mass is including the mass of helium gas in the balloon. To calculate
maximum load, mass of helium must subtracted from the maximum mass so,
π‘šπ‘šπ‘Žπ‘₯,πΏπ‘œπ‘Žπ‘‘ = π‘šπ‘šπ‘Žπ‘₯ − π‘šβ„Žπ‘’ = 607.304[π‘˜π‘”] − 86.77[π‘˜π‘”] = 520.6[π‘˜π‘”]
1
Problem 3:
πœŒπ‘œπ‘–π‘™
⁄𝜌
𝐻2 π‘œ = 0.85
OIL
h=5 m
Analysis:
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ENSC 388
Assignment # 1
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h=5 m
Starting with point (1) and adding terms gh as
WATER
we go down,
𝑃1 + πœŒπ‘œπ‘–π‘™ π‘”β„Žπ‘œπ‘–π‘™ + 𝜌𝐻2 π‘œ π‘”β„Žπ»2 π‘œ = 𝑃2
πœŒπ‘œπ‘–π‘™ π‘”β„Žπ‘œπ‘–π‘™ + 𝜌𝐻2 π‘œ π‘”β„Žπ»2 π‘œ = 𝑃2 − 𝑃1
2
𝜌
𝑃2 − 𝑃1 = ( π‘œπ‘–π‘™⁄𝜌𝐻 π‘œ β„Žπ‘œπ‘–π‘™ + β„Žπ»2 π‘œ ) 𝜌𝐻2 π‘œ 𝑔
2
Substituting values,
𝜌𝐻2 π‘œ = 1000 [
π‘˜π‘”⁄
]
π‘š3
𝑃2 − 𝑃1 = (0.85[−] × 5[π‘š] + 5[π‘š])1000 [
π‘˜π‘”⁄
] × 9.81 [π‘š⁄ 2 ]
π‘š3
𝑠
= 90.742[π‘˜π‘ƒπ‘Ž]
Notes (1): Always substitute the numerical value at the last step.
Note (2): Write all the dimensions in your solution; check both sides of
relationships for unit and dimension homogeneity.
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ENSC 388
Assignment # 1
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