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DEVAPRAKASAM DEIVASAGAYAM
Professor of Mechanical Engineering
Room:11, LW, 2nd Floor
School of Mechanical and Building Sciences
Email: devaprakasam.d@vit.ac.in, dr.devaprakasam@gmail.com
MEE1002: Engineering Mechanics (2:1:0:0:3)
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Wedges are simple machines used
to raise large stone blocks and
other heavy loads. These loads can
be raised by applying to the wedge
a force usually considerably
smaller than the weight of the load.
In addition, because of the friction
between the surfaces in contact, a
properly shaped wedge will remain
in place after being forced under
the load. Wedges can thus be used
advantageously to make small
adjustments in the position of
heavy pieces of machinery.
Static or Dynamic?
• Static Friction
• Kinetic Friction
tanφs= Fm/N=µs N/N
tanφk=Fk/N=µk N/N
P
N
Ff
W
Ff
P
Motion
Fm
Fk
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Static or Dynamic?
P
N
Ff
W
W
θ
θ
N
W sinθ
W cosθ
N cosθ
N sinθ
Case 1: Ff>P, (µsN>P) No Motion
Case 2: Fm=P, (µsN=P) Impending Motion
Case3: Fk<P, (µkN<P) Motion
Case 1: Ff>P, (µs N Sinθ>P) , No Motion
Case 2: Fm=P, (µs N Sinθ=P), Impending
Motion
Case3: Fk<P, (µk N Sinθ<P) Motion,
θ
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
θ
θ
y
x
F
N
Maximum Friction Force
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
x
Maximum Friction Force
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
y
θ
θ
x
F
N
Maximum
Friction Force
Actual Friction Force
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Dry Friction
y
Maximum
Friction Force
Actual Friction Force
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
It is convenient to replace the normal force N and the
friction force F by their resultant R.
Applied force P has a horizontal component Px which tends to move
the block, the force R will have a horizontal component F and, thus, will
form an angle φ with the normal to the surface
If Px is increased until
motion becomes
impending, the angle
between R and the vertical
grows and reaches a
maximum value.This value
is called the angle of static
friction and is denoted by
φs .
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
If motion actually takes place, the magnitude of the friction
force drops to Fk; similarly, the angle f between R and N
drops to a lower value φk, called the angle of kinetic friction
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Two 8° wedges of negligible weight are used to move and position the 800-kg
block. Knowing that the coefficient of static friction is 0.30 at all surfaces of
contact, determine the smallest force P that should be applied as shown to one of
the wedges.
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
WEDGES
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
WEDGES
W
8°
8°
16.7°
R1
R2
16.7°
16.7°
R2
R1
16.7°
24.7°
α
7848N
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
WEDGES
R3
R1
90°-16.7°
β
P
90°-24.7°
R3
R1
P
16.7° 24.7°
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
WEDGES
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
WEDGES
W
16.7°
R1
R2
16.7°
16.7°
R2
R1
16.7°
16.7°
α
7848N
`
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
WEDGES
R3
R1
90°-24.7°
β
P
90°-16.7°
R3
R1
P
16.7°
24.7°
16.7°8°
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Ladder
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Ladder
NC
FC
NA
FA
NB
FB
NB
FB
40lb 40lb
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Ladder
;
;
;
;
;
;
;
;
;
=0;
6
;
;
;
17.143;
;
=0;
;
;
Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
Ladder

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Mechanical Engineering Professor Devaprakasam's Lecture on Wedges and Friction

  • 1. DEVAPRAKASAM DEIVASAGAYAM Professor of Mechanical Engineering Room:11, LW, 2nd Floor School of Mechanical and Building Sciences Email: devaprakasam.d@vit.ac.in, dr.devaprakasam@gmail.com MEE1002: Engineering Mechanics (2:1:0:0:3) Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
  • 2. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Wedges are simple machines used to raise large stone blocks and other heavy loads. These loads can be raised by applying to the wedge a force usually considerably smaller than the weight of the load. In addition, because of the friction between the surfaces in contact, a properly shaped wedge will remain in place after being forced under the load. Wedges can thus be used advantageously to make small adjustments in the position of heavy pieces of machinery.
  • 3. Static or Dynamic? • Static Friction • Kinetic Friction tanφs= Fm/N=µs N/N tanφk=Fk/N=µk N/N P N Ff W Ff P Motion Fm Fk
  • 4. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 5. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 6. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 7. Static or Dynamic? P N Ff W W θ θ N W sinθ W cosθ N cosθ N sinθ Case 1: Ff>P, (µsN>P) No Motion Case 2: Fm=P, (µsN=P) Impending Motion Case3: Fk<P, (µkN<P) Motion Case 1: Ff>P, (µs N Sinθ>P) , No Motion Case 2: Fm=P, (µs N Sinθ=P), Impending Motion Case3: Fk<P, (µk N Sinθ<P) Motion, θ
  • 8. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
  • 9. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 10. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 11. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 12. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction θ θ y x F N Maximum Friction Force
  • 13. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction x Maximum Friction Force
  • 14. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction
  • 15. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction y θ θ x F N Maximum Friction Force Actual Friction Force
  • 16. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Dry Friction y Maximum Friction Force Actual Friction Force
  • 17. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 It is convenient to replace the normal force N and the friction force F by their resultant R. Applied force P has a horizontal component Px which tends to move the block, the force R will have a horizontal component F and, thus, will form an angle φ with the normal to the surface If Px is increased until motion becomes impending, the angle between R and the vertical grows and reaches a maximum value.This value is called the angle of static friction and is denoted by φs .
  • 18. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 If motion actually takes place, the magnitude of the friction force drops to Fk; similarly, the angle f between R and N drops to a lower value φk, called the angle of kinetic friction
  • 19. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
  • 20. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
  • 21. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933
  • 22. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Two 8° wedges of negligible weight are used to move and position the 800-kg block. Knowing that the coefficient of static friction is 0.30 at all surfaces of contact, determine the smallest force P that should be applied as shown to one of the wedges.
  • 23. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 WEDGES
  • 24. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 WEDGES W 8° 8° 16.7° R1 R2 16.7° 16.7° R2 R1 16.7° 24.7° α 7848N
  • 25. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 WEDGES R3 R1 90°-16.7° β P 90°-24.7° R3 R1 P 16.7° 24.7°
  • 26. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 WEDGES
  • 27. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 WEDGES W 16.7° R1 R2 16.7° 16.7° R2 R1 16.7° 16.7° α 7848N `
  • 28. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 WEDGES R3 R1 90°-24.7° β P 90°-16.7° R3 R1 P 16.7° 24.7° 16.7°8°
  • 29. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Ladder
  • 30. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Ladder NC FC NA FA NB FB NB FB 40lb 40lb
  • 31. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Ladder ; ; ; ; ; ; ; ; ; =0; 6 ; ; ; 17.143; ; =0; ; ;
  • 32. Devaprakasam D, Email: devaprakasam.d@vit.ac.in, Ph: +91 9786553933 Ladder