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ES-101-Cluster-ABC-Sample-Problems

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ES 101
Mechanics of Particles and Rigid Bodies
Additional Sample Problems (Cluster ABC)
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Prepared by: Stephanie Joy B. Carag
ADDITION OF VECTORS
• Parallelogram Law
o This states that two forces acting on a particle
may be replaced by a single force, called their
resultant , obtained by drawing the diagonal of
the parallelogram which has sides equal to the
given forces.
• Triangle Rule
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Cluster ABC
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RECTANGULAR COMPONENTS OF A FORCE
• In many problems it will be found desirable to resolve a force into two components
which are perpendicular to each other.
• Scalar: Rectangular components (Fx and Fy)
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UNIT VECTORS
• In many problems it will be found desirable to
resolve a force into two components which are
perpendicular to each other.
• Unit vectors (i and j)
𝐹π‘₯ = 𝐹cosπœƒ
𝐹𝑦 = 𝐹sinπœƒ
𝐹 = 𝐹π‘₯ i + 𝐹𝑦 j
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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Cluster ABC
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PROBLEM 2.36 Knowing that the tension in rope AC is 365 N, determine the
resultant of the three forces exerted at point C of post BC.
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PROBLEM 2.36 Knowing that the tension in rope AC is 365 N, determine the
resultant of the three forces exerted at point C of post BC.
Free-Body Diagram
25
C
24
3
7
500N
5
4
TAC= 365N
200N
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PROBLEM 2.36 Knowing that the tension in rope AC is 365 N, determine the
resultant of the three forces exerted at point C of post BC.
Free Body Diagram
Cable force AC:
𝐹π‘₯ = − 365𝑁
500N
𝐹𝑦 = − 365𝑁
960
= −240N
1460
1100
= −275N
1460
500N Force:
𝐹π‘₯ = 500𝑁
TAC= 365N
200N
𝐹𝑦 = 500𝑁
24
= 480N
25
7
= 140N
25
200N Force:
𝐹π‘₯ = 200𝑁
𝐹𝑦 = − 200𝑁
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4
= 160N
5
3
= −120N
5
ES 101 Mechanics of Particles and Rigid Bodies
Cluster ABC
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PROBLEM 2.36 Knowing that the tension in rope AC is 365 N, determine the resultant of the
three forces exerted at point C of post BC.
Cable force AC:
𝐹π‘₯ = − 365𝑁
𝐹𝑦 = − 365𝑁
Resultant:
960
= −240N
1460
1100
= −275N
1460
𝑅π‘₯ = ෍ 𝐹π‘₯ = −240𝑁 + 480𝑁 + 160𝑁 = 400N
𝑅𝑦 = ෍ 𝐹𝑦 = −275𝑁 + 140𝑁 − 120𝑁 = −255N
500N Force:
𝐹π‘₯ = 500𝑁
𝐹𝑦 = 500𝑁
24
= 480N
25
24
= 140N
25
200N Force:
𝐹π‘₯ = 200𝑁
𝐹𝑦 = − 200𝑁
4
= 160N
5
3
= −120N
5
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R = 400N i − 255N j
𝑅=
𝑅π‘₯ 2 + 𝑅𝑦 2 =
(400𝑁)2 + −255𝑁
2
= πŸ’πŸ•πŸ’. πŸ‘πŸ•π‘΅
255
400
∝= 32.5°
tan ∝ =
Rx = 400N i
∝
Ry = -255N j
ES 101 Mechanics of Particles and Rigid Bodies
Cluster ABC
R = 474.37N
22
Note: Three force body, i.e., a rigid body subjected to three forces or, more generally, a rigid body subjected to forces acting at only three points
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RECTILINEAR MOTION OF PARTICLES
• Uniform Rectilinear Motion
π‘₯ = π‘₯0 + 𝑣𝑑
• Uniformly Accelerated Rectilinear Motion
𝑣 = 𝑣0 + π‘Žπ‘‘
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MOTION OF SEVERAL PARTICLES
• Consider two particles A and B moving along the same straight line
• If the position coordinates xA and xB are measured from the same origin, the difference xB
- xA defines the relative position coordinate of B with respect to A and is denoted by xB/A.
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Problem 3.35 Given the vectors P = 3i - j + 2k, Q = 4i + 5j - 3k, and S = -2i +
3j - k, compute the scalar products P · Q, P · S, and Q · S.
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Problem 3.35 Given the vectors P = 3i - j + 2k, Q = 4i + 5j - 3k, and S = -2i +
3j - k, compute the scalar products P · Q, P · S, and Q · S.
𝑃 βˆ™ 𝑄 = (3𝑖 − 𝑗 + 2π‘˜) βˆ™ (4𝑖 + 5𝑗 − 3π‘˜)
𝑃 βˆ™ 𝑄 = 3 4 + −1 5 + 2 −3
𝑃 βˆ™ 𝑄 = 12 − 5 − 6 = 1
𝑃 βˆ™ 𝑆 = (3𝑖 − 𝑗 + 2π‘˜) βˆ™ (−2𝑖 + 3𝑗 − π‘˜)
𝑃 βˆ™ 𝑆 = 3 −2 + −1 3 + 2 −1
𝑃 βˆ™ 𝑆 = −6 − 3 − 2 = −11
𝑄 βˆ™ 𝑆 = (4𝑖 + 5𝑗 − 3π‘˜) βˆ™ (−2𝑖 + 3𝑗 − π‘˜)
𝑄 βˆ™ 𝑆 = 4 −2 + 5 3 + −3 −1
𝑃 βˆ™ 𝑆 = −8 + 15 + 3 = 10
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RECTANGULAR COMPONENTS OF 3D FORCES:
Using 2 points on its LOA
Consider a force F along line of action, line MN.
• When a segment of the line of action is given,
𝒅 = 𝑑π‘₯ π’ŠΤ¦ + 𝑑𝑦 𝒋Ԧ + 𝑑𝑧 π’Œ
where
𝑑π‘₯ = π‘₯2 − π‘₯1
𝒅 =𝑑=
𝑑𝑦 = 𝑦2 − 𝑦1
𝑑𝑧 = 𝑧2 − 𝑧1
𝑑π‘₯ 2 + 𝑑𝑦 2 + 𝑑𝑧 2
• 𝝀 the unit vector of its line of action is then determined as
𝒅
π‘₯2 − π‘₯1 π’ŠΤ¦ + 𝑦2 − 𝑦1 𝒋Ԧ + 𝑧2 − 𝑧1 π’Œ
𝝀 =
=
𝒅
π‘₯2 − π‘₯1 2 + 𝑦2 − 𝑦1 2 + 𝑧2 − 𝑧1 2
• The force can then be expressed as
𝐹
𝑭 = 𝐹𝝀 =
𝑑π‘₯ π’ŠΤ¦ + 𝑑𝑦 𝒋Ԧ + 𝑑𝑧 π’Œ
𝑑
𝑑𝑦
𝑑π‘₯
𝑑𝑧
𝑭 = 𝐹 π’ŠΤ¦ + 𝐹 𝒋Ԧ + 𝐹 π’Œ
𝑑
𝑑
𝑑
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REFLECT: This means that the direction cosines
are related to the line of action such that
𝑭 = 𝐹π‘₯ π’ŠΤ¦ + 𝐹𝑦 𝒋Ԧ + 𝐹𝑧 π’Œ
𝑑π‘₯
cos πœƒπ‘₯ =
𝑑
𝑑𝑦
cos πœƒπ‘¦ =
𝑑
ES 101 Mechanics of Particles and Rigid Bodies
Cluster ABC
𝑑𝑧
cos πœƒπ‘§ =
𝑑
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Coordinates:
A (16, 0, -11) ft
B (0, 8, 0) ft
C (0, 8, -27) ft
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𝒅 =𝑑=
A (16, 0, -11) ft
B (0, 8, 0) ft
C (0, 8, -27) ft
𝑑π‘₯ 2 + 𝑑𝑦 2 + 𝑑𝑧 2
AB < -16, 8, 11 >
AC < -16, 8, -16 >
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A (16, 0, -11) ft
B (0, 8, 0) ft
C (0, 8, -27) ft
AB < -16, 8, 11 >
AC < -16, 8, -16 >
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
A (960, 240, 0) mm
B (0, 0, 380) mm
C (0, 0, -320) mm
D (0, 960, -220) mm
෍ 𝐹𝐴 = 0 ∢ 𝑇𝐴𝐡 + 𝑇𝐴𝐢 + 𝑇𝐴𝐷 + 𝑃 = 0
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
A (960, 240, 0) mm
B (0, 0, 380) mm
C (0, 0, -320) mm
D (0, 960, -220) mm
Express the vectors into components <dx, dy, dz> or dxiΜ‚ + dyjΜ‚ + dzkΜ‚ :
𝐴𝐡 < −960, −240, 380 > π‘šπ‘š
𝐴𝐢 < −960, −240, −320 > π‘šπ‘š
𝐴𝐷 < −960, 720, −220 > π‘šπ‘š
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
A (960, 240, 0) mm
B (0, 0, 380) mm
C (0, 0, -320) mm
D (0, 960, -220) mm
𝐴𝐡 < −960, −240, 380 > π‘šπ‘š
𝐴𝐢 < −960, −240, −320 > π‘šπ‘š
𝐴𝐷 < −960, 720, −220 > π‘šπ‘š
Identify the magnitude of the vector
𝐴𝐡 =
−960
2
+ −240
2
+ 380
𝒅 =𝑑=
2
𝑑 π‘₯ 2 + 𝑑𝑦 2 + 𝑑𝑧 2
= πŸπŸŽπŸ”πŸŽ π’Žπ’Ž
AB = 1060 mm
AC = 1040 mm
AD = 1220 mm
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
A (960, 240, 0) mm
B (0, 0, 380) mm
C (0, 0, -320) mm
D (0, 960, -220) mm
𝐴𝐡 < −960, −240, 380 > π‘šπ‘š
𝐴𝐢 < −960, −240, −320 > π‘šπ‘š
𝐴𝐷 < −960, 720, −220 > π‘šπ‘š
AB = 1060 mm
AC = 1040 mm
AD = 1220 mm
𝑑
𝑑
𝑑
ΰ·‘
Determine the unit vector πœ†ΰ΄± = π‘₯ π’ŠΖΈ + 𝑦 𝒋Ƹ + 𝑧 π’Œ
𝑑
𝑑
𝑑
960
240
380
ΰ·‘
π’ŠΖΈ −
𝒋Ƹ +
π’Œ
1060
1060
1060
960
240
320
ΰ·‘
𝝀𝑨π‘ͺ = −
π’ŠΖΈ −
𝒋Ƹ −
π’Œ
1040
1040
1040
960
720
220
ΰ·‘
𝝀𝑨𝑫 = −
π’ŠΖΈ +
𝒋Ƹ −
π’Œ
1220
1220
1220
𝝀𝑨𝑩 = −
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
Force components:
960
240
380
ΰ·‘
π’ŠΖΈ −
𝒋Ƹ +
π’Œ
1060
1060
1060
960
240
320
ΰ·‘
𝑻𝑨π‘ͺ = 𝑇𝐴𝐢 πœ†π΄πΆ = 𝑇𝐴𝐢 −
π’ŠΖΈ −
𝒋Ƹ −
π’Œ
1040
1040
1040
960
720
220
ΰ·‘
𝑻𝑨𝑫 = 𝑇𝐴𝐷 πœ†π΄π· = 305 𝑁 −
π’ŠΖΈ +
𝒋Ƹ −
π’Œ
1220
1220
1220
𝑻𝑨𝑩 = 𝑇𝐴𝐡 πœ†π΄π΅ = 𝑇𝐴𝐡 −
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Problem 2.107 Three cables are connected at A, where the forces P and Q
are applied as shown. Knowing that Q = 0, find the value of P for which the
tension in cable AD is 305 N.
Force components:
960
240
380
ΰ·‘
π’ŠΖΈ −
𝒋Ƹ +
π’Œ
1060
1060
1060
960
240
320
ΰ·‘
𝑻𝑨π‘ͺ = 𝑇𝐴𝐢 πœ†π΄πΆ = 𝑇𝐴𝐢 −
π’ŠΖΈ −
𝒋Ƹ −
π’Œ
1040
1040
1040
960
720
220
ΰ·‘
𝑻𝑨𝑫 = 𝑇𝐴𝐷 πœ†π΄π· = 305 𝑁 −
π’ŠΖΈ +
𝒋Ƹ −
π’Œ
1220
1220
1220
𝑻𝑨𝑩 = 𝑇𝐴𝐡 πœ†π΄π΅ = 𝑇𝐴𝐡 −
Summation of forces:
෍ 𝐹𝐴 = 0 ∢ 𝑇𝐴𝐡 + 𝑇𝐴𝐢 + 𝑇𝐴𝐷 + 𝑃 = 0
෍ 𝐹π‘₯ = 0: −
960
960
−960
𝑇𝐴𝐡 −
𝑇𝐴𝐢 +
1060
1040
1220
305 + 𝑃 = 0
෍ 𝐹𝑦 = 0: −
240
240
720
𝑇𝐴𝐡 −
𝑇𝐴𝐢 +
1060
1040
1220
305 = 0
෍ 𝐹𝑧 = 0:
380
320
−220
𝑇𝐴𝐡 −
𝑇𝐴𝐢 +
1060
1040
1220
305 = 0
𝑻𝑨𝑩 = πŸ’πŸ’πŸ”. πŸ•πŸπ‘΅
𝑻𝑨π‘ͺ = πŸ‘πŸ’πŸ. πŸ•πŸπ‘΅
𝑷 = πŸ—πŸ”πŸŽ 𝑡
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Problem 2.72 Determine (a) the x, y, and z components of the 750-N force, (b) the
angles θx, θy, and θz that the force forms with the coordinate axes
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Problem 2.72 Determine (a) the x, y, and z components of the 750-N force, (b) the
angles θx, θy, and θz that the force forms with the coordinate axes
πΉβ„Ž = 𝐹 sin 35
πΉβ„Ž = 750𝑁 sin 35
πΉβ„Ž = 430.18 𝑁
𝐹π‘₯ = πΉβ„Ž cos 25
𝐹π‘₯ = 430.18𝑁 cos 25
𝐹π‘₯ = 389.88 𝑁
𝐹𝑦 = 𝐹 cos 35
𝐹𝑦 = 750𝑁 cos 35
𝐹𝑦 = 614.36𝑁
𝐹π‘₯ 389.88𝑁
=
𝐹
750𝑁
𝐹𝑦 614.36𝑁
cos πœƒπ‘¦ = =
𝐹
750𝑁
𝐹𝑧 181.802𝑁
cos πœƒπ‘§ = =
𝐹
750𝑁
cos πœƒπ‘₯ =
πœƒπ‘₯ = 58.7°
πœƒπ‘¦ = 35.0°
πœƒπ‘§ = 76.0°
Fh
𝐹𝑧 = πΉβ„Ž sin 25
𝐹𝑧 = 430.18𝑁 sin 25
𝐹𝑧 = 181.802𝑁
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STATIC AND KINETIC FRICTION
Fs
𝐹𝑠 = πœ‡π‘  𝑁
πΉπ‘˜ = πœ‡π‘˜ 𝑁
μs = coefficient of static friction
μk =coefficient of kinetic friction
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ANGLES OF FRICTION
tan ∅𝑠 = πœ‡π‘ 
tan ∅π‘˜ = πœ‡π‘˜
Ο•s = angle of static friction
Ο•k = angle of kinetic friction
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Problem 8.6 Knowing that the coefficient of friction between the 25-kg block and the
incline is μs = 0.25, determine (a) the smallest value of P required to start the block moving
up the incline, (b) the corresponding value of b.
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Problem 8.6 Knowing that the coefficient of friction between the 25-kg block and the
incline is μs = 0.25, determine (a) the smallest value of P required to start the block moving
up the incline, (b) the corresponding value of b.
Free-Body Diagram (Impending motion up)
P
P
β
β
30°
FS
30°
W
Ο•s
R
W
N
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Problem 8.6 Knowing that the coefficient of friction between the 25-kg block and the
incline is μs = 0.25, determine (a) the smallest value of P required to start the block moving
up the incline, (b) the corresponding value of b.
P
β
Ο•
30° s
W
P
a
30°
R
b
π‘Š = π‘šπ‘”
π‘Š = 25 π‘˜π‘” 9.81π‘š/𝑠 2
π‘Š = 245.25𝑁
tan ∅𝑠 = πœ‡π‘ 
∅𝑠 = tan−1 0.25
∅𝑠 = 14°
W = mg
d
R
For minimum P, P ⊥ R
𝑃
π‘Š
𝑃 = π‘Š sin 30° + ∅𝑠
𝑃 = 245.25 𝑁 sin 30° + 14.04°
sin 30° + ∅𝑠 =
π‘·π’Žπ’Šπ’ = πŸπŸ•πŸπ‘΅
Consider β–³acd,
90 = (30 + Ο•s )+ [90 - (30+ β)]
β = Ο•s
β = πŸπŸ’°
c
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Problem 8.11 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between
two blocks and zero between block B and incline, determine the value of πœƒ for which
motion is impending.
Block A
Impending motion:
y
T
x
πœƒ
෍ 𝐹𝑦 = 0: 𝑁1 − π‘Š1 cos πœƒ = 0
𝑁1 = 20 9.81 cos πœƒ
𝑁1 = 196.2 cos πœƒ
F1= πœ‡π‘  N1
N1
W1 = m1g
෍ 𝐹π‘₯ = 0: −𝑇 + 𝐹1 + π‘Š1 s𝑖𝑛 πœƒ = 0
𝑇 = 𝐹1 + π‘Š1 s𝑖𝑛 πœƒ
𝑇 = 0.15 196.2 cos πœƒ + 196.2 sin θ
𝑇 = 29.43 cos πœƒ + 196.2 sin θ
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Problem 8.11 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between
two blocks and zero between block B and incline, determine the value of πœƒ for which
motion is impending.
Block B
Impending motion:
y
T
x
෍ 𝐹𝑦 = 0: 𝑁2 − 𝑁1 − π‘Š2 cos πœƒ = 0
F1= πœ‡π‘  N1
πœƒ
𝑁2 = 196.2 cos πœƒ + 30(9.81) cos πœƒ
𝑁2 = 490.5 cos θ
F2= 0
N2
෍ 𝐹π‘₯ = 0: −𝑇 − 𝐹1 − 𝐹2 + π‘Š2 s𝑖𝑛 πœƒ = 0
W2 = m2g
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𝑇 = −𝐹1 − 0 + π‘Š2 s𝑖𝑛 πœƒ
𝑇 = −0.15 196.2 cos πœƒ + 30(9.81) sin θ
𝑇 = −29.43 cos πœƒ + 294.3 sin θ
ES 101 Mechanics of Particles and Rigid Bodies
Cluster ABC
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Problem 8.11 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between
two blocks and zero between block B and incline, determine the value of πœƒ for which
motion is impending.
Eq (1): 𝑇 = 29.43 cos πœƒ + 196.2 sin θ
Eq (2): 𝑇 = −29.43 cos πœƒ + 294.3 sin θ
Eq (2) – Eq (1):
0 = −58.86 cos πœƒ + 98.1 sin θ
58.86 cos πœƒ = 98.1 sin θ
58.86
98.1
𝛉 = πŸ‘πŸ°
tan θ =
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Problem 8.12 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between all
surfaces of contact, determine the value of πœƒ for which motion is impending.
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Problem 8.12 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between all
surfaces of contact, determine the value of πœƒ for which motion is impending.
Block A
Impending motion:
y
T
x
πœƒ
෍ 𝐹𝑦 = 0: 𝑁1 − π‘Š1 cos πœƒ = 0
𝑁1 = 20 9.81 cos πœƒ
𝑁1 = 196.2 cos πœƒ
F1= πœ‡π‘  N1
N1
W1 = m1g
෍ 𝐹π‘₯ = 0: −𝑇 + 𝐹1 + π‘Š1 s𝑖𝑛 πœƒ = 0
𝑇 = 𝐹1 + π‘Š1 s𝑖𝑛 πœƒ
𝑇 = 0.15 196.2 cos πœƒ + 196.2 sin θ
𝑇 = 29.43 cos πœƒ + 196.2 sin θ
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Problem 8.12 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between all
surfaces of contact, determine the value of πœƒ for which motion is impending.
Block B
Impending motion:
y
T
x
πœƒ
N2
෍ 𝐹𝑦 = 0: 𝑁2 − 𝑁1 − π‘Š2 cos πœƒ = 0
F1= πœ‡π‘  N1
𝑁2 = 196.2 cos πœƒ + 30(9.81) cos πœƒ
𝑁2 = 490.5 cos θ
F2= πœ‡π‘  N2
෍ 𝐹π‘₯ = 0: −𝑇 − 𝐹1 − 𝐹2 + π‘Š2 s𝑖𝑛 πœƒ = 0
W2 = m2g
𝑇 = −𝐹1 − 𝐹2 + π‘Š2 s𝑖𝑛 πœƒ
𝑇 = −0.15 196.2 cos πœƒ − 0.15(490.5 cos θ) + 30(9.81) sin θ
𝑇 = −29.43 cos πœƒ − 73.575 cos θ + 294.3 sin θ
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Problem 8.12 The 20-kg block A and the 30-kg block B are supported by an incline that is
held in the position shown. Knowing that the coefficient of static friction is 0.15 between all
surfaces of contact, determine the value of πœƒ for which motion is impending.
Eq (1): 𝑇 = 29.43 cos πœƒ + 196.2 sin θ
Eq (2): 𝑇 = −29.43 cos πœƒ − 73.575 cos πœƒ + 294.3 sin θ
Eq (2) – Eq (1):
0 = −132.435 cos πœƒ + 98.1 sin θ
132.435 cos πœƒ = 98.1 sin θ
132.435
98.1
𝛉 = πŸ“πŸ‘°
tan θ =
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REFERENCE
• Vector mechanics for engineers: statics and dynamics / Ferdinand Beer . . . [et al.]. —
10th ed (2013)
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