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Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

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Lecture 24 ENGR-1100 Introduction to Engineering Analysis
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Page 1: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Lecture 24

ENGR-1100 Introduction to Engineering Analysis

Page 2: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Today’s Lecture Outline

Dry friction (Coulomb friction)

Page 3: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Friction

Friction forces oppose the tendency of contacting surfaces to slip one relative to the other.

Dry friction- the tangential component of the contact force.

Page 4: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Friction

Forces have to be concurrent in order to be in equilibrium.

Page 5: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Friction forces as a function of P

Maximum value of friction forces is called the limiting value of static friction. This condition is also called the impending motion.

Page 6: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Tip vs. slip

Body Tips

F1

P2>P1

F2

Page 7: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

The magnitude of the friction forces

Fmax=sN

Where s is the coefficient of static friction.It is independent of normal forces and area of contact.

F<sNThe general case for equilibrium condition

Once the body starts to slip

F=kN k is the coefficient of dynamic friction

k < s

Page 8: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

The Resultant of the friction and normal forces

R= N2+F2 tan = F/N

At the point of impending motion:

R= N2+F2max = N2+(sN)2 = N 1+ s

2

tan s= F/N= sN/N= s s is the angle of static friction

s

Page 9: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Gravity forces in inclined surfaces

sFor equilibrium:

Page 10: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Example 9-4

Two blocks with masses mA = 20 kg and mB = 80 kg are connected

with a flexible cable that passes over a frictionless pulley as shown in Fig. P9-4. The coefficient of friction between the blocks is 0.25. If motion of the blocks is impending, determine the coefficient of friction between block B and the inclined surface and the tension in the cable between the two blocks.

Page 11: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Solution

Fy = An - 196.14 cos(35) = 0

An = 160.67 N

For impending motion of the block A: (Af = s.An)

+ Fx = -T + 0.25(160.67) + 196.14 sin 35 = 0

T = 152.67 N

Free body diagram for block A

Page 12: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Free body diagram for block B:

WB = mB.g = 80 (9.807) = 784.56 N

Block B weight:

Fy = Bn - 160.67 - 784.56 cos 35 = 0

Bn = 803.34 N

= Bf/Bn= 257.17/803.34 = 0.320

Bf = 257.17 N

Fx = - Bf - 40.17 - 152.67 + 784.56 sin 35 = 0

Page 13: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Class Assignment: Exercise set P9-1please submit to TA at the end of the lecture

Determine the horizontal force P required to start moving the 250-lb block shown in Fig. P9-1 up the inclined surface. The coefficient of friction between the inclined surface and the block is s = 0.30.

P = 265.29 lb 265.3b

Page 14: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

SolutionFor impending motion: 

Ff = Fn = 0.30Fn

Fy = Fn cos 30 - Ff sin 30 -W= Fn cos 30 - 0.30Fn sin 30 - 250 = 0

Free body diagram for the block:

Fn = 349.15 lb

Fx = P - Fn sin 30 - Ff cos 30= P - 349.15 sin 30 - 0.30 (349.15) cos 30 = 0

P = 265.29 lb 265.3b

Page 15: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Class Assignment: Exercise set P9-36please submit to TA at the end of the lecture

The masses of blocks A and B of Fig. P9-36 are mA = 40 kg

and mB = 85 kg. If the coefficient of friction is 0.25 for both

surfaces, determine the force P required to cause impending motion of block B.

P 935 N

Page 16: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Solution

From a free-body diagram for the block A when motion is impending:

Af = Af (max) = A An = 0.25 An

WA = mAg = 40 (9.807) = 392.28 N

Fy = An cos 45 + Af sin 45 - WA

= An cos 45 + 0.25 An sin 45 - 392.28 = 0

An= 443.81 N

Af= 0.25 An = 110.95 N

Page 17: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

From a free-body diagram for the block B when motion is impending:

Fx = P cos 20-WB sin 45-Af -Bf

= P cos 20-833.60 sin 45-110.95-0.25Bn = 0

WB = mBg = 85 (9.807) = 833.60 N

Bf = Bf (max) = Bn = 0.25Bn

Fy = P sin 20 - WB cos 45 - An + Bn

= P sin 20 - 833.60 cos 45 - 443.81 + Bn = 0

P 935 N

Page 18: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Class Assignment: Exercise set P9-3please submit to TA at the end of the lecture

Workers are pulling a 400 lb crate up an incline as shown in Fig. P9-3. The coefficient of friction between the crate and the surface is 0.20, and the rope on which the workers are pulling is horizontal.(a) Determine the force P that the workers must exert to start sliding the crate up the incline.(b) If one of the workers lets go of the rope for a moment, determine the minimum force the other workers must exert to keep the crate from sliding back down the incline.

a) P=197.8 lb

b) P=25.8lb

Page 19: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

A 120 lb girl is walking up a 48-lb uniform beam as shown in Fig. P9-21. Determine how far up the beam the girl can walk before the beam starts to slip if(a)The coefficient of friction is 0.20 at all surfaces(b)The coefficient of friction at the bottom end of the beam isincreased to 0.40 by placing a piece of rubber between the beam and the floor.

a) x = 3.21 ftb) x = 6.26 ft

Class Assignment: Exercise set P9-3please submit to TA at the end of the lecture

Page 20: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

Solution(a) For a free-body diagram for thebeam when motion is impending:

Ar = An = 0.2An

Bf= Bn = 0.2Bn

= tan-16/8 = 36.87

68

Fh = Bn sin 36.87 - 0.2Bn cos 36.87 - 0.2An = 0

+ Fy = Bn cos 36.87 + 0.2Bn sin 36.87 + An - 120 - 48 = 0Solving yields: An = 118.46 lb; Bn = 53.85 lb

+ MA = 48(6) cos 36.87 + 120(x) cos 36.87 - 53.85(10) = 0

x = 3.209 ft 3.21 ft

Page 21: Lecture 24 ENGR-1100 Introduction to Engineering Analysis.

(b) For a free-body diagram for the beam when motion is impending:

Ar = An = 0.4An

Bf= Bn = 0.2Bn

+ Fh = Bn sin 36.87 - 0.2Bn cos 36.87 - 0.4An = 0

+ Fy = Bn cos 36.87 + 0.2Bn sin 36.87 + An - 120 - 48 = 0

Solving yields:An = 91.49 lb; Bn = 83.17 lb

+ MA = 48(6) cos 36.87 + 120(x) cos 36.87 - 83.17(10) = 0

x = 6.264 ft 6.26 ft


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