Quiz 1_solution

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ENSC 283 Quiz #1
Jan. 27, 2009
Name: ……………………………………… Student ID:………………………………..
Time: 45 minutes or less. Develop answers on available place. The quiz has 5% (bonus) of
the total mark. Closed books & closed notes.
Problem 1 (50%):
A square, side dimension a (m), has its top edge H (m) below the water surface. It is on
angle θ and its bottom is hinged as shown in the figure below. Develop a relationship for
the force F needed to just open the gate.
F
H
Water
a
θ
Hinge
Hint: start with drawing a free-body-diagram of the gate. Also:
𝑦𝐢𝑃 = −π›Ύπ‘ π‘–π‘›πœƒ
𝐼π‘₯π‘₯
M. Bahrami
π‘Ž4
=
12
ENSC 283 (S 09)
𝐼π‘₯π‘₯
𝑝𝐢𝐺 𝐴
𝐴 = π‘Ž2
Quiz #1
1
Solution:
The first step is to sketch a free-body diagram of the gate so the forces and distances are
clearly identified. It is done in the following figure.
H
F
FR
.
CG
|𝑦𝐢𝑃 |
θ
Fx
Fy
The force 𝐹𝑅 is calculated to be
𝐹𝑅 = π›Ύβ„ŽπΆπΊ 𝐴 = 𝛾(𝐻 +
π‘Ž sin πœƒ
2
(Eq.1)
)π‘Ž2
We will take moments about the hinge so that it will not be necessary to calculate the
forces 𝐹π‘₯ and 𝐹𝑦 .
π‘Ž
(Eq.2)
𝐹𝑅 × [2 − |𝑦𝐢𝑃 |] = 𝐹 × π‘Ž
where, |𝑦𝐢𝑃 | is the distance between the center of pressure (CP) and the center of gravity
(CG). |𝑦𝐢𝑃 | can be written as:
|𝑦𝐢𝑃 | = π›Ύπ‘ π‘–π‘›πœƒ
M. Bahrami
𝐼π‘₯π‘₯
𝐼π‘₯π‘₯ sin πœƒ π‘Ž4
sin πœƒ
π‘Ž2 sin πœƒ
=
=
=
𝑝𝐢𝐺 𝐴
β„ŽπΆπΊ 𝐴
12 (𝐻 + π‘Ž sin πœƒ)π‘Ž2 12(𝐻 + π‘Ž sin πœƒ)
2
2
ENSC 283 (S 09)
Quiz #1
(Eq.3)
2
Substituting |𝑦𝐢𝑃 | into Eq.2, the force F is found.
𝐹=
π‘Ž
𝐹𝑅 × [2 − |𝑦𝐢𝑃 |]
π‘Ž
=
𝛾(𝐻 +
π‘Ž sin πœƒ 2 π‘Ž
|𝑦 |]
2 )π‘Ž [2 − 𝐢𝑃
π‘Ž
(Eq.4)
Simplifying the above equation, we get:
𝐹=
M. Bahrami
π›Ύπ‘Ž2 (3𝐻 + π‘Ž sin πœƒ)
6
ENSC 283 (S 09)
(Eq.5)
Quiz #1
3
Problem 2 (50%):
It is said that Archimedes discovered the buoyancy laws when asked by King Hiero of
Syracuse to determine whether his new crown was pure gold (SG = 19.3). Archimedes
measured the weight of the crown in air to be 11.8 N and its weight in water to be 10.9 N.
Was it pure gold?
Hint: the buoyancy is the difference between air weight and underwater weight.
𝐹𝐡 = 𝛾𝑉
Solution:
The buoyancy is the difference between air weight and underwater weight:
(Eq.1)
𝐹𝐡 = π‘Šπ‘–π‘› π‘Žπ‘–π‘Ÿ − π‘Šπ‘–π‘› π‘€π‘Žπ‘‘π‘’π‘Ÿ = π›Ύπ‘€π‘Žπ‘‘π‘’π‘Ÿ π‘‰π‘π‘Ÿπ‘œπ‘€π‘› = 11.8 𝑁 − 10.9 𝑁 = 0.9 𝑁
where, π‘Šπ‘–π‘› π‘Žπ‘–π‘Ÿ and π‘Šπ‘–π‘› π‘€π‘Žπ‘‘π‘’π‘Ÿ are the weight of the crown in air and water, respectively.
The weight of the crown in air can be expressed as:
π‘Šπ‘–π‘› π‘Žπ‘–π‘Ÿ = (𝑆𝐺)π›Ύπ‘€π‘Žπ‘‘π‘’π‘Ÿ π‘‰π‘π‘Ÿπ‘œπ‘€π‘›
(Eq.2)
Substituting Eq.2 into Eq.1, we get:
π‘Šπ‘–π‘› π‘€π‘Žπ‘‘π‘’π‘Ÿ = π›Ύπ‘€π‘Žπ‘‘π‘’π‘Ÿ π‘‰π‘π‘Ÿπ‘œπ‘€π‘› (𝑆𝐺 − 1) = 𝐹𝐡 (𝑆𝐺 − 1)
(Eq.3)
Thus, the specific gravity of the crown can be written as:
𝑆𝐺 = 1 +
M. Bahrami
π‘Šπ‘–π‘› π‘€π‘Žπ‘‘π‘’π‘Ÿ
𝐹𝐡
=1+
10.9
0.9
(Eq.4)
= πŸπŸ‘. 𝟏𝟏 (𝒏𝒐𝒕 𝒑𝒖𝒓𝒆 π’ˆπ’π’π’…)
ENSC 283 (S 09)
Quiz #1
4
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