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Mechanics of Deformable Bodies: Solved Stress Problems

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MECHANICS OF DEFORMABLE
BODIES
PROBLEM SET NO.1
Submitted by:
Submitted to:
Average Normal Stress
Problem 1.1
A shop crane consists of a boom AC that’s supported by a pin at A and by
a rectangular tension bar BD, as shown in Fig.1. Details of the pin joints at A and
B are shown in views a-a and b-b, respectively. The tension bar BD has a width
w=1.5in. and a thickness t=0.5in. If the vertical load at C is P=5kips, what is the
average tensile stress in the bar BD?
Given:
1. w=1.5in.
2. t=0.5in
3. P=5kips
Required:
1. The average tensile stress in the bar BD.
Solution:
+↑ ∑ 𝐹𝑦 = 0
π‘‡π‘ π‘–π‘›πœƒ − 𝑃 = 0 eq.1
+→ ∑ 𝐹π‘₯ = 0
π‘‡π‘π‘œπ‘ πœƒ = 0 eq.2
LBD= √(6𝑓𝑑)2 + (4𝑓𝑑)2 = √36 + 16 = √52 = 7.21𝑓𝑑
πœƒ = tan−1 (
π‘œπ‘π‘
4𝑓𝑑
) = π‘‘π‘Žπ‘›−1 (
) = 33.69°
π‘Žπ‘‘π‘—
6𝑓𝑑
subs. eq.1:
𝑇𝑠𝑖𝑛(33.69°) − 𝑃 = 0
𝑇=
𝑃
5π‘˜π‘–π‘π‘ 
=
0.555 0.555
𝑇 = 9.01π‘˜π‘–π‘π‘ 
subs eq.2:
π‘‡π‘π‘œπ‘ πœƒ = 0
9.01π‘˜π‘–π‘π‘  × 0.832 = 7.49π‘˜π‘–π‘π‘ 
𝑇 = 7.49π‘˜π‘–π‘π‘ 
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
𝑇
𝜎=𝐴
𝐴 = 𝑀𝑑 = 1.5𝑖𝑛 × 0.5𝑖𝑛 = 0.75𝑖𝑛2
𝜎=
9.01π‘˜π‘–π‘π‘ 
0.75𝑖𝑛2
𝝈 = 𝟏𝟐. πŸŽπŸπŸ‘πŸ‘π’Œπ’”π’Š
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
Problem 1.2
Two solid circular rods are welded to a plate at B to form a single rod, as shown
in Fig.1. Consider the 30kN force at B to be uniformly distributed around the
circumference of the collar at B and the 10kN load at C to be applied at the centroid
of the end cross section. Determine the axial stress in each portion of the rod.
Given:
1. Pb=30kN
2. Pc=10kN
3. d₁=20mm
4. dβ‚‚=15mm
Required:
1. the axial stress in each
portion of the rod.
Solution:
𝐅
𝐀
FAB= πŸ‘πŸŽπ’Œπ‘΅(Tensile) = 30,000N
FBC= πŸπŸŽπ’Œπ‘΅(Compressive) = 10,000N
𝛔=
For AB:
π‘¨πŸ =
𝛔=
π…π‘«πŸ 𝝅(πŸπŸŽπ’Žπ’Ž)𝟐
=
= πŸ‘πŸπŸ’. πŸπŸ”π’Žπ’ŽπŸ
πŸ’
πŸ’
𝐅
πŸ‘πŸŽ, 𝟎𝟎𝟎𝐍
=
= πŸ—πŸ“. πŸ’πŸ—πŸπŸ•πŒππš
𝐀 πŸ‘πŸπŸ’. πŸπŸ”π¦π¦πŸ
For BC:
𝛑(πŸπŸ“π¦π¦)𝟐
𝟐
𝐀 =
= πŸπŸ•πŸ”. πŸ•πŸπ¦π¦πŸ
πŸ’
𝛔=
𝟏𝟎, 𝟎𝟎𝟎𝐍
= πŸ“πŸ”. πŸ“πŸ–πŸ—πŸ—πŒππš
πŸπŸ•πŸ”. πŸ•πŸπ¦π¦πŸ
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
Problem 1.3
The plate has a width of 0.5m. if the stress distribution at the support varies as
shown. Determine the force P applied to the plate and the distance d to where it is
applied.
Given:
1. w=0.5m
2. L=4m
3. δ=(15x½) MPa
4. δ=30MPa
Required:
1. The force P applied to the
plate and the distance d to
where it is applied.
Solution:
+↑ ∑ 𝐹𝑦 = 0
𝐿
𝑃 = ∫ 𝜎(π‘₯) βˆ™ 𝑀𝑑π‘₯
0
4
1
𝑃 = ∫ 15π‘₯ 2 × 0.5𝑑π‘₯
0
4
1
𝑃 = 7.5 ∫ π‘₯ 2 𝑑π‘₯
0
2 3 4
2
𝑃 = 7.5 [ π‘₯ 2 ] = 7.5 ( × 8) = 40π‘˜π‘
3
0
3
+β†Ί ∑ 𝑀π‘₯ = 0
𝐿
𝑀 = ∫ π‘₯ βˆ™ 𝜎(π‘₯) βˆ™ 𝑀𝑑π‘₯
0
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
4
3
𝑀 = 7.5 ∫ π‘₯ 2 𝑑π‘₯
0
2 5 4
2
𝑀 = 7.5 [ π‘₯ 2 ] = 7.5 ( × 32) = 96π‘˜π‘ βˆ™ π‘š
5
0
5
𝑀𝑝 = 𝑃𝑑; 𝑀𝑝 = 𝑀
𝑃𝑑 = 𝑀
40π‘˜π‘ × π‘‘ = 96π‘˜π‘ βˆ™ π‘š
𝑑=
96π‘˜π‘ βˆ™ π‘š
= 2.4π‘š
40π‘˜π‘
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
Problem 1.4
The frame shown consists of four wooden members, ABC, DEF, BE, and CF.
Knowing that each member has a 2x4in. rectangular cross section and that each pin
has a ½in. diameter, determine the maximum value of the average normal stress (a) in
member BE, (b) in member CF.
Given:
1. W=480lb
2. d=½in
3. A=2x4in
Required:
1. The maximum
value of the
average normal
stress (a) in
member BE, (b)
in member CF.
Solution:
At Joint C:
+↑ ∑ 𝐹𝑦 = 0
𝐹 CF π‘ π‘–π‘›πœƒCF−π‘Š = 0
𝐹 CF π‘ π‘–π‘›πœƒCF= 480𝑙𝑏
The angle for πœƒCF:
πœƒ = tan−1 (
15𝑖𝑛
) = 26.57°
30𝑖𝑛
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
480𝑙𝑏
𝐹 CF=
sin(26.57°)
=
480
0.447
= 1074.2𝑙𝑏
+→ ∑ 𝐹π‘₯ = 0
𝐹 CF π‘π‘œπ‘ πœƒCF−𝐹 BC π‘π‘œπ‘ πœƒBC= 0
At Joint B:
+↑ ∑ 𝐹𝑦 = 0
𝐹 BE π‘ π‘–π‘›πœƒBE−𝐹 BC π‘ π‘–π‘›πœƒBC= 0
45𝑖𝑛
πœƒBE= tan−1 (30𝑖𝑛) = 56.31
+→ ∑ 𝐹π‘₯ = 0
𝐹 BE π‘π‘œπ‘ πœƒBE−𝐹 AB π‘π‘œπ‘ πœƒAB= 0
The angle for πœƒBE:
45𝑖𝑛
πœƒBE= tan−1 (30𝑖𝑛) = 56.31
The angle for πœƒBC:
45𝑖𝑛
πœƒBC= tan−1 (40𝑖𝑛) = 48.37°
𝐹 BE=
πΉπ΅πΆπ‘ π‘–π‘›πœƒπ΅πΆ
π‘ π‘–π‘›πœƒπ΅πΈ
Assuming 𝐹 BC= 480𝑙𝑏
𝑭BE
πŸ’πŸ–πŸŽ×π’”π’Šπ’(πŸ’πŸ–.πŸ‘πŸ•°)
𝝈=
π’”π’Šπ’(πŸ“πŸ”.πŸ‘πŸ°)
=
πŸ’πŸ–πŸŽ×𝟎.πŸ•πŸ’πŸ–
𝟎.πŸ–πŸ‘πŸ
= πŸ’πŸ‘πŸ. πŸ“π’π’ƒ
𝑭
𝑨
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
𝑨 = πŸπ’Šπ’ × πŸ’π’Šπ’ = πŸ–π’Šπ’πŸ
For member BE:
𝜎=
𝐹 431.5𝑙𝑏
=
= 53.9375𝑝𝑠𝑖
𝐴
8𝑖𝑛2
For member CF:
𝜎=
𝐹 1074.2𝑙𝑏
=
= 134.275𝑝𝑠𝑖
𝐴
8𝑖𝑛2
Solved Problems in Mechanics of Deformable Bodies
1
Average Normal Stress
Problem 1.5
An aircraft tow bar is positioned by means of a single hydraulic cylinder
connected by a 25mm diameter steel rod to two identical arm and wheel units DEF. The
mass of the entire tow bar is 200 kg, and its center of gravity is located at G. For the
position shown, determine the normal stress in the rod.
Given:
1. D=25mm
2. m=200kg
Required:
1. The normal
stress in the
rod.
Solution:
𝜎=
𝐹
𝐴
𝐹 = π‘šπ‘” = 200π‘˜π‘” ×
9.81π‘š
= 1962𝑁
𝑠2
𝐴=
πœ‹π·2 πœ‹(25π‘šπ‘š)2
=
= 490.87π‘šπ‘š2
4
4
𝜎=
𝐹
1962𝑁
=
𝐴 490.87π‘šπ‘š2
𝝈 = πŸ’π‘΄π‘·π’‚
Solved Problems in Mechanics of Deformable Bodies
1
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