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King Fahd University of Petroleum & Minerals. Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 11. Sir Isaac Newton 1642-1727. Proposed fundamental laws that are the basis of modern mechanics 3 laws of motion law of gravitation. Newton ’ s laws. - PowerPoint PPT PresentationTRANSCRIPT
King Fahd University of Petroleum &
MineralsMechanical Engineering
Dynamics ME 201BY
Dr. Meyassar N. Al-HaddadLecture # 11
Sir Isaac Newton1642-1727
Proposed fundamental laws that are the basis of modern mechanics
3 laws of motionlaw of gravitation
Newton’s lawsLaw of inertia a body in motion will stay in motion and a body at rest will
stay at rest unless acted upon by a net external force.
Law of force-acceleration A particle acted upon by an unbalanced force F experiences an acceleration a that has the same direction as the force and a magnitude that is directly proportional to the force
Law of action-reaction for every action, there is an equal and opposite reaction mg = FN
Law of gravitation - all bodies are attracted to one another with a force proportional to the product of their masses and inversely proportional to the square of the distance between them.
221
rmmGF
amF
13.2 The Equation of Motion
• Free-Body diagram (Force Diagram)
• Kinetic diagram (acceleration Diagram)
aF m
13.3 Equation of Motion for a System of Particles
iiii m
m
afF
aF
G
iii
m
m
aF
aF
Internal forces cancel each other
13.4 Equations of Motion: Rectangular Coordinates
• When the net force is projected to separate coordinate axes the Newton’s second law still holds
)kji(kji
aF
zyxzyx aaamFFF
m
zz
yy
xx
maF
maF
maF
Free Body Diagram Method
•Draw each object separately
•Draw all the forces acting on that object
•Get x and y components of all the forces to calculate the net force
•Apply Newton’s second law to get acceleration
•Use the acceleration in any motion analysis and establish a Kinetic Diagram
ma
Normal & Frictional Force
F
Ff
FN
Action-Reaction forces -mg = FN
mg
Static Friction ( s )
• Static friction – parallel force on the surface when there is no relative motion between the 2 objects
• Static friction force can vary from zero to Maximum
The coefficient of static friction is material dependent.
StaticFf = sFN
DynamicFf = kFN
Applied external force
Frict
ion
Kinetic Friction ( k )
• Kinetic friction – parallel force on the surface when there is relative motion between the 2 objects
• Kinetic friction force is always the same
• The coefficient of Kinetic friction
• is material dependent.
NkFF μf
StaticFf = sFN
DynamicFf = kFN
Applied external force
Frict
ion
Spring Force
• Spring force
• k : spring stiffness (N/m)• s : stretched or
compressed length
ksFs
olls
ol l
s
• m = 2 kg• y = 1m• smooth• a = ?
maFmg s sin
2219sin
9053cosx5.0x3coscos
m/s.θmksga
N.θksθFN sc
ma
Example 13-4
0cos sc FN
13537501tan
507507501
1
22
..
θ
m...S
x
ymg
N Nk
Problem
NNN
369020cos81.940
;0 yF
xx maF mamgNk sin
0cos mgN
2/66.5
4020sin81.940)369(25.0
sma
a
x
x
a? =
Example 13-5
m A= 3 kgm B= 5 kgFrom restvB= ? In 2 second
yy maFAaT 32981
Block A
yy maFBaT 52.196
Block B
lss BA 2 02 BA 02 BA aa
taBo
Same
Same ٍshould be
VA? =
2Sc + SA = L 0 = 2ac + aA aA = -2ac
ca
ccx
y
amgTNmaF
NNNF
20030sin25.0:
1699030cos81.9*200:0
Problem
mg Ama
)/(62.42 smsaV AA
)2(12525.1226
12581.9*125
A
AA
aT
aTmaFy
NTsmasma
aaaa
aa
A
A
A
c
cc
c
c
1004)/(777.1)/(888.0
500200250200622
200981)12525.1226(25.849)1()2(
22
Review
• Example 13.1• Example 13.2• Example 13.3• Example 13.4