Presentation is loading. Please wait.

Presentation is loading. Please wait.

CHARACTERISTICS OF DRY FRICTION & PROBLEMS INVOLVING DRY FRICTION

Similar presentations


Presentation on theme: "CHARACTERISTICS OF DRY FRICTION & PROBLEMS INVOLVING DRY FRICTION"— Presentation transcript:

1 CHARACTERISTICS OF DRY FRICTION & PROBLEMS INVOLVING DRY FRICTION
Today’s Objective: Students will be able to: a) Understand the characteristics of dry friction. b) Draw a FBD including friction. c) Solve problems involving friction. In-Class Activities: Check Homework, if any Reading Quiz Applications Characteristics of Dry Friction Problems Involving Dry Friction Concept Quiz Group Problem Solving Attention Quiz Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

2 1. A friction force always acts _____ to the contact surface.
READING QUIZ 1. A friction force always acts _____ to the contact surface. A) Normal B) At 45° C) Parallel D) At the angle of static friction 2. If a block is stationary, then the friction force acting on it is ________ . A)  s N B) = s N C)  s N D) = k N Answers: 1. C 2. A Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

3 APPLICATIONS In designing a brake system for a bicycle, car, or any other vehicle, it is important to understand the frictional forces involved. For an applied force on the brake pads, how can we determine the magnitude and direction of the resulting friction force? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

4 APPLICATIONS (continued)
The rope is used to tow the refrigerator. In order to move the refrigerator, is it best to pull up as shown, pull horizontally, or pull downwards on the rope? What physical factors affect the answer to this question? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

5 CHARACTERISTICS OF DRY FRICTION (Section 8.1)
Friction is defined as a force of resistance acting on a body which prevents or retards slipping of the body relative to a second body. Experiments show that frictional forces act tangent (parallel) to the contacting surface in a direction opposing the relative motion or tendency for motion. For the body shown in the figure to be in equilibrium, the following must be true: F = P, N = W, and W*x = P*h. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

6 CHARACTERISTICS OF DRY FRICTION (continued)
To study the characteristics of the friction force F, let us assume that tipping does not occur (i.e., “h” is small or “a” is large). Then we gradually increase the magnitude of the force P. Typically, experiments show that the friction force F varies with P, as shown in the right figure above. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

7 CHARACTERISTICS OF DRY FRICTION (continued)
The maximum friction force is attained just before the block begins to move (a situation that is called “impending motion”). The value of the force is found using Fs = s N, where s is called the coefficient of static friction. The value of s depends on the twoo materials in contact. Once the block begins to move, the frictional force typically drops and is given by Fk = k N. The value of k (coefficient of kinetic friction) is less than s . Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

8 CHARACTERISTICS OF DRY FRICTION (continued)
It is also very important to note that the friction force may be less than the maximum friction force. So, just because the object is not moving, don’t assume the friction force is at its maximum of Fs = s N unless you are told or know motion is impending! Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

9 DETERMING s EXPERIMENTALLY
If the block just begins to slip, the maximum friction force is Fs = s N, where s is the coefficient of static friction. Thus, when the block is on the verge of sliding, the normal force N and frictional force Fs combine to create a resultant Rs From the figure, tan s = ( Fs / N ) = (s N / N ) = s Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

10 DETERMING s EXPERIMENTALLY (continued)
A block with weight w is placed on an inclined plane. The plane is slowly tilted until the block just begins to slip. The inclination, s, is noted. Analysis of the block just before it begins to move gives (using Fs = s N): +  Fy = N – W cos s = 0 +  FX = S N – W sin s = 0 Using these two equations, we get s = (W sin s ) / (W cos s ) = tan s This simple experiment allows us to find the S between two materials in contact. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

11 PROBLEMS INVOLVING DRY FRICTION (Section 8.2)
Steps for solving equilibrium problems involving dry friction: 1. Draw the necessary free body diagrams. Make sure that you show the friction force in the correct direction (it always opposes the motion or impending motion). 2. Determine the number of unknowns. Do not assume F = S N unless the impending motion condition is given. 3. Apply the equations of equilibrium and appropriate frictional equations to solve for the unknowns. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

12 IMPENDING TIPPING versus SLIPPING
For a given W and h of the box, how can we determine if the block will slide or tip first? In this case, we have four unknowns (F, N, x, and P) and only three E-of-E. Hence, we have to make an assumption to give us another equation (the friction equation!). Then we can solve for the unknowns using the three E-of-E. Finally, we need to check if our assumption was correct. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

13 IMPENDING TIPPING versus SLIPPING (continued)
Assume: Slipping occurs Known: F = s N Solve: x, P, and N Check: 0  x  b/2 Or Assume: Tipping occurs Known: x = b/2 Solve: P, N, and F Check: F  s N Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

14 EXAMPLE Given: A uniform ladder weighs 30 lb. The vertical wall is smooth (no friction). The floor is rough and s = 0.2. Find: Whether it remains in this position when it is released. Plan: a) Draw a FBD. b) Determine the unknowns. c) Make any necessary friction assumptions. d) Apply E-of-E (and friction equations, if appropriate ) to solve for the unknowns. e) Check assumptions, if required. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

15 EXAMPLE (continued) NB FBD of the ladder 12 ft FA NA 5 ft
There are three unknowns: NA, FA, NB. 30 lb NB 12 ft 5 ft NA FA FBD of the ladder   FY = NA – 30 = 0 ; so NA = 30 lb +  MA = 30 ( 5 ) – NB( 24 ) = 0 ; so NB = 6.25 lb +   FX = 6.25 – FA = 0 ; so FA = 6.25 lb Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

16 EXAMPLE (continued) Now check the friction force to see if the ladder slides or stays. Fmax = s NA = 0.2 * 30 lb = 6 lb Since FA = 6.25 lb  Ffriction max = 6 lb, the pole will not remain stationary. It will move. 30 lb NB 12 ft 5 ft NA FA FBD of the ladder Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

17 C) P(C) D) Can not be determined
CONCEPT QUIZ 1. A 100 lb box with a wide base is pulled by a force P and s = Which force orientation requires the least force to begin sliding? A) P(A) B) P(B) C) P(C) D) Can not be determined P(A) P(B) P(C) 100 lb 2. A ladder is positioned as shown. Please indicate the direction of the friction force on the ladder at B. A)  B)  C) D) A B Answer: 1. A 2. C Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

18 Given: Refrigerator weight = 180 lb, s = 0.25
GROUP PROBLEM SOLVING Given: Refrigerator weight = 180 lb, s = 0.25 Find: The smallest magnitude of P that will cause impending motion (tipping or slipping) of the refrigerator. Plan: a) Draw a FBD of the refrigerator. b) Determine the unknowns. c) Make friction assumptions, as necessary. d) Apply E-of-E (and friction equation as appropriate) to solve for the unknowns. e) Check assumptions, as required. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

19 GROUP PROBLEM SOLVING (continued)
X 1.5 ft 180 lb F FBD of the refrigerator P N 3 ft 4 ft There are four unknowns: P, N, F and x. First, let’s assume the refrigerator slips. Then the friction equation is F = s N = N. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

20 GROUP PROBLEM SOLVING (continued)
X 1.5 ft 180 lb F FBD of the refrigerator P N 3 ft 4 ft P +   FX = P – N = 0 +   FY = N – = 0 These two equations give: P = 45 lb and N = 180 lb +  MO = 45 (4) (x) = 0 Check: x =  so OK! Refrigerator slips as assumed at P = 45 lb Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

21 ATTENTION QUIZ 1. A 10 lb block is in equilibrium. What is the magnitude of the friction force between this block and the surface? A) 0 lb B) 1 lb C) 2 lb D) 3 lb  S = 0.3 2 lb 2. The ladder AB is postioned as shown. What is the direction of the friction force on the ladder at B. A) B) C)  D)  A B Answers are: 1. C 2. D Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

22 End of the Lecture Let Learning Continue
Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections

23 WEDGES AND FRICTIONAL FORCES ON FLAT BELTS
Today’s Objectives: Students will be able to: a) Determine the forces on a wedge. b) Determine the tensions in a belt. In-Class Activities: Check Homework, if any Reading Quiz Applications Analysis of a Wedge Analysis of a Belt Concept Quiz Group Problem Solving Attention Quiz Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

24 1. A wedge allows a ______ force P to lift a _________ weight W.
READING QUIZ 1. A wedge allows a ______ force P to lift a _________ weight W. A) (large, large) B) (small, small) C) (small, large) D) (large, small) W 2. Considering friction forces and the indicated motion of the belt, how are belt tensions T1 and T2 related? A) T1 > T B) T1 = T2 C) T1 < T D) T1 = T2 e Answers: 1. C 2. C All quizzes (Reading, Attention, Concept): The questions are numbered.One space is left between the numeral and question text. Do not use automatic bullets as this is not compatible with ’97 version of PowerPoint Answer choices are listed by upper case alphabets A, B, C, D, enclosed by right parenthesis. Single space is Left between the Alphabet and the Answer choice. The choices have hanging indentation aligned with the starting of the question text. For multiple fill up the blanks,answers are enclosed in parenthesis. (see #1 above) Figures/Pictures are positioned on the right side of the slide. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

25 How can we determine the force required to pull the wedge out?
APPLICATIONS Wedges are used to adjust the elevation or provide stability for heavy objects such as this large steel pipe. How can we determine the force required to pull the wedge out? When there are no applied forces on the wedge, will it stay in place (i.e., be self-locking) or will it come out on its own? Under what physical conditions will it come out? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

26 APPLICATIONS (continued)
Belt drives are commonly used for transmitting the torque developed by a motor to a wheel attached to a pump, fan or blower. How can we decide if the belts will function properly, i.e., without slipping or breaking? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

27 APPLICATIONS (continued)
In the design of a band brake, it is essential to analyze the frictional forces acting on the band (which acts like a belt). How can you determine the tensions in the cable pulling on the band? Also from a design perspective, how are the belt tension, the applied force P and the torque M, related? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

28 ANALYSIS OF A WEDGE A wedge is a simple machine in which a small force P is used to lift a large weight W. W To determine the force required to push the wedge in or out, it is necessary to draw FBDs of the wedge and the object on top of it. It is easier to start with a FBD of the wedge since you know the direction of its motion. Note that: a) the friction forces are always in the direction opposite to the motion, or impending motion, of the wedge; b) the friction forces are along the contacting surfaces; and, c) the normal forces are perpendicular to the contacting surfaces. As noted earlier, important text is given a blue color and underlined. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

29 ANALYSIS OF A WEDGE (continued)
Next, a FBD of the object on top of the wedge is drawn. Please note that: a) at the contacting surfaces between the wedge and the object the forces are equal in magnitude and opposite in direction to those on the wedge; and, b) all other forces acting on the object should be shown. To determine the unknowns, we must apply EofE,  Fx = 0 and  Fy = 0, to the wedge and the object as well as the impending motion frictional equation, F = S N.

30 ANALYSIS OF A WEDGE (continued)
Now of the two FBDs, which one should we start analyzing first? We should start analyzing the FBD in which the number of unknowns are less than or equal to the number of EofE and frictional equations.

31 ANALYSIS OF A WEDGE (continued)
NOTE: If the object is to be lowered, then the wedge needs to be pulled out. If the value of the force P needed to remove the wedge is positive, then the wedge is self-locking, i.e., it will not come out on its own. W

32 BELT ANALYSIS Consider a flat belt passing over a fixed curved surface with the total angle of contact equal to  radians. If the belt slips or is just about to slip, then T2 must be larger than T1 and the motion resisting friction forces. Hence, T2 must be greater than T1. Detailed analysis (please refer to your textbook) shows that T2 = T1 e   where  is the coefficient of static friction between the belt and the surface. Be sure to use radians when using this formula!!

33 Find: The smallest force P needed to pull out the wedge.
EXAMPLE Given: The crate weighs 300 lb and S at all contacting surfaces is 0.3. Assume the wedges have negligible weight. Find: The smallest force P needed to pull out the wedge. Plan: 1. Draw a FBD of the crate. Why do the crate first? 2. Draw a FBD of the wedge. 3. Apply the E-of-E to the crate. 4. Apply the E-of-E to wedge. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

34 Solving the above two equations, we get
EXAMPLE (continued) The FBDs of crate and wedge are shown in the figures. Applying the EofE to the crate, we get NB 300 lb FB=0.3NB FC=0.3NC NC 15º FD=0.3ND ND P FBD of Crate FBD of Wedge Known forces are indicated by blue color arrow, Unknown forces indicated by yellow color. The thickness of arrow lines are 2 1/4 pt. Bolden the Decimal Point Symbols used in the equations are from the Symbols library. do not use sentence case on ‘cos’ and ‘sin’, they are to be in lower case. +  FX = NB – 0.3NC = 0 +  FY = NC – NB = 0 Solving the above two equations, we get NB = lb = 82.6 lb, NC = lb = 275 lb Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

35 Applying the E-of-E to the wedge, we get
EXAMPLE (continued) NB = 82.6 lb 300 lb FB=0.3NB FC=0.3NC NC = 275 lb 15º NC FD=0.3ND ND P FBD of Crate FBD of Wedge Applying the E-of-E to the wedge, we get +  FY = ND cos 15 ND sin 15 – = 0; ND = lb = 264 lb +  FX = 0.3(263.7) + 0.3(263.7)cos 15 – 0.3(263.7)cos 15 – P = 0; P = lb Known forces are indicated by blue color arrow, Unknown forces indicated by yellow color. The thickness of arrow lines are 2 1/4 pt. Bolden the Decimal Point Symbols used in the equations are from the Symbols library. do not use sentence case on ‘cos’ and ‘sin’, they are to be in lower case. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

36 A) Be lifted up B) Slide down C) Not be lifted up D) Not slide down
CONCEPT QUIZ 1. Determine the direction of the friction force on object B at the contact point between A and B. A)  B)  C) D) 2. The boy (hanging) in the picture weighs 100 lb and the woman weighs 150 lb. The coefficient of static friction between her shoes and the ground is The boy will ______ ? A) Be lifted up B) Slide down C) Not be lifted up D) Not slide down Answers: 1. C 2. C The maximum force she can apply before she slides is 150 (0.6) = 90 lb. This will not be enough to lift the boy up as she needs to apply more than 100 lb to lift the boy up. Without knowing the coefficient of friction between the cliff and the rope, we can not say whether the boy will slide down or not. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

37 Given: Blocks A and B weigh 50 lb and 30 lb, respectively.
GROUP PROBLEM SOLVING Given: Blocks A and B weigh 50 lb and 30 lb, respectively. Find: The smallest weight of cylinder D which will cause the loss of static equilibrium. Plan:

38 GROUP PROBLEM SOLVING (continued)
Plan: 1. Consider two cases: a) both blocks slide together, and, b) block B slides over the block A. 2. For each case, draw a FBD of the block(s). 3. For each case, apply the EofE to find the force needed to cause sliding. 4. Choose the smaller P value from the two cases. 5. Use belt friction theory to find the weight of block D.

39 GROUP PROBLEM SOLVING (continued)
Case a (both blocks sliding together): +  FY = N – 80 = 0 N = 80 lb +  FX = 0.4 (80) – P = 0 P = lb P B A N F=0.4 N 30 lb 50 lb

40 GROUP PROBLEM SOLVING (continued)
 +  Fy = N cos 20 N sin 20 – 30 = N = lb  +  Fx = – P ( 26.2 ) cos 20 – 26.2 sin 20 = P = lb 20º 30 lb 0.6 N P N Case b (block B slides over A): Case b has the lowest P (case a was 32 lb) and thus will occur first. Next, using a frictional force analysis of belt, we get WD = P e   = e 0.5 ( 0.5  ) = lb A Block D weighing 12.7 lb will cause the block B to slide over the block A.

41 A) The wedge B) The block
ATTENTION QUIZ 1. When determining the force P needed to lift the block of weight W, it is easier to draw a FBD of ______ first. A) The wedge B) The block C) The horizontal ground D) The vertical wall W 2. In the analysis of frictional forces on a flat belt, T2 = T1 e  . In this equation,  equals ______ . A) Angle of contact in degrees B) Angle of contact in radians C) Coefficient of static friction D) Coefficient of kinetic friction Answers: 1.A 2.B Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

42 End of the Lecture Let Learning Continue
In the last slide add the ‘home’ action button Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

43 WEDGES AND FRICTIONAL FORCES ON FLAT BELTS
Today’s Objectives: Students will be able to: a) Determine the forces on a wedge. b) Determine the tensions in a belt. In-Class Activities: Check Homework, if any Reading Quiz Applications Analysis of a Wedge Analysis of a Belt Concept Quiz Group Problem Solving Attention Quiz Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

44 1. A wedge allows a ______ force P to lift a _________ weight W.
READING QUIZ 1. A wedge allows a ______ force P to lift a _________ weight W. A) (large, large) B) (small, small) C) (small, large) D) (large, small) W 2. Considering friction forces and the indicated motion of the belt, how are belt tensions T1 and T2 related? A) T1 > T B) T1 = T2 C) T1 < T D) T1 = T2 e Answers: 1. C 2. C All quizzes (Reading, Attention, Concept): The questions are numbered.One space is left between the numeral and question text. Do not use automatic bullets as this is not compatible with ’97 version of PowerPoint Answer choices are listed by upper case alphabets A, B, C, D, enclosed by right parenthesis. Single space is Left between the Alphabet and the Answer choice. The choices have hanging indentation aligned with the starting of the question text. For multiple fill up the blanks,answers are enclosed in parenthesis. (see #1 above) Figures/Pictures are positioned on the right side of the slide. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

45 How can we determine the force required to pull the wedge out?
APPLICATIONS Wedges are used to adjust the elevation or provide stability for heavy objects such as this large steel pipe. How can we determine the force required to pull the wedge out? When there are no applied forces on the wedge, will it stay in place (i.e., be self-locking) or will it come out on its own? Under what physical conditions will it come out? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

46 APPLICATIONS (continued)
Belt drives are commonly used for transmitting the torque developed by a motor to a wheel attached to a pump, fan or blower. How can we decide if the belts will function properly, i.e., without slipping or breaking? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

47 APPLICATIONS (continued)
In the design of a band brake, it is essential to analyze the frictional forces acting on the band (which acts like a belt). How can you determine the tensions in the cable pulling on the band? Also from a design perspective, how are the belt tension, the applied force P and the torque M, related? Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

48 ANALYSIS OF A WEDGE A wedge is a simple machine in which a small force P is used to lift a large weight W. W To determine the force required to push the wedge in or out, it is necessary to draw FBDs of the wedge and the object on top of it. It is easier to start with a FBD of the wedge since you know the direction of its motion. Note that: a) the friction forces are always in the direction opposite to the motion, or impending motion, of the wedge; b) the friction forces are along the contacting surfaces; and, c) the normal forces are perpendicular to the contacting surfaces. As noted earlier, important text is given a blue color and underlined. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

49 ANALYSIS OF A WEDGE (continued)
Next, a FBD of the object on top of the wedge is drawn. Please note that: a) at the contacting surfaces between the wedge and the object the forces are equal in magnitude and opposite in direction to those on the wedge; and, b) all other forces acting on the object should be shown. To determine the unknowns, we must apply EofE,  Fx = 0 and  Fy = 0, to the wedge and the object as well as the impending motion frictional equation, F = S N.

50 ANALYSIS OF A WEDGE (continued)
Now of the two FBDs, which one should we start analyzing first? We should start analyzing the FBD in which the number of unknowns are less than or equal to the number of EofE and frictional equations.

51 ANALYSIS OF A WEDGE (continued)
NOTE: If the object is to be lowered, then the wedge needs to be pulled out. If the value of the force P needed to remove the wedge is positive, then the wedge is self-locking, i.e., it will not come out on its own. W

52 BELT ANALYSIS Consider a flat belt passing over a fixed curved surface with the total angle of contact equal to  radians. If the belt slips or is just about to slip, then T2 must be larger than T1 and the motion resisting friction forces. Hence, T2 must be greater than T1. Detailed analysis (please refer to your textbook) shows that T2 = T1 e   where  is the coefficient of static friction between the belt and the surface. Be sure to use radians when using this formula!!

53 Find: The smallest force P needed to pull out the wedge.
EXAMPLE Given: The crate weighs 300 lb and S at all contacting surfaces is 0.3. Assume the wedges have negligible weight. Find: The smallest force P needed to pull out the wedge. Plan: 1. Draw a FBD of the crate. Why do the crate first? 2. Draw a FBD of the wedge. 3. Apply the E-of-E to the crate. 4. Apply the E-of-E to wedge. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

54 Solving the above two equations, we get
EXAMPLE (continued) The FBDs of crate and wedge are shown in the figures. Applying the EofE to the crate, we get NB 300 lb FB=0.3NB FC=0.3NC NC 15º FD=0.3ND ND P FBD of Crate FBD of Wedge Known forces are indicated by blue color arrow, Unknown forces indicated by yellow color. The thickness of arrow lines are 2 1/4 pt. Bolden the Decimal Point Symbols used in the equations are from the Symbols library. do not use sentence case on ‘cos’ and ‘sin’, they are to be in lower case. +  FX = NB – 0.3NC = 0 +  FY = NC – NB = 0 Solving the above two equations, we get NB = lb = 82.6 lb, NC = lb = 275 lb Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

55 Applying the E-of-E to the wedge, we get
EXAMPLE (continued) NB = 82.6 lb 300 lb FB=0.3NB FC=0.3NC NC = 275 lb 15º NC FD=0.3ND ND P FBD of Crate FBD of Wedge Applying the E-of-E to the wedge, we get +  FY = ND cos 15 ND sin 15 – = 0; ND = lb = 264 lb +  FX = 0.3(263.7) + 0.3(263.7)cos 15 – 0.3(263.7)cos 15 – P = 0; P = lb Known forces are indicated by blue color arrow, Unknown forces indicated by yellow color. The thickness of arrow lines are 2 1/4 pt. Bolden the Decimal Point Symbols used in the equations are from the Symbols library. do not use sentence case on ‘cos’ and ‘sin’, they are to be in lower case. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

56 A) Be lifted up B) Slide down C) Not be lifted up D) Not slide down
CONCEPT QUIZ 1. Determine the direction of the friction force on object B at the contact point between A and B. A)  B)  C) D) 2. The boy (hanging) in the picture weighs 100 lb and the woman weighs 150 lb. The coefficient of static friction between her shoes and the ground is The boy will ______ ? A) Be lifted up B) Slide down C) Not be lifted up D) Not slide down Answers: 1. C 2. C The maximum force she can apply before she slides is 150 (0.6) = 90 lb. This will not be enough to lift the boy up as she needs to apply more than 100 lb to lift the boy up. Without knowing the coefficient of friction between the cliff and the rope, we can not say whether the boy will slide down or not. Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

57 Given: Blocks A and B weigh 50 lb and 30 lb, respectively.
GROUP PROBLEM SOLVING Given: Blocks A and B weigh 50 lb and 30 lb, respectively. Find: The smallest weight of cylinder D which will cause the loss of static equilibrium. Plan:

58 GROUP PROBLEM SOLVING (continued)
Plan: 1. Consider two cases: a) both blocks slide together, and, b) block B slides over the block A. 2. For each case, draw a FBD of the block(s). 3. For each case, apply the EofE to find the force needed to cause sliding. 4. Choose the smaller P value from the two cases. 5. Use belt friction theory to find the weight of block D.

59 GROUP PROBLEM SOLVING (continued)
Case a (both blocks sliding together): +  FY = N – 80 = 0 N = 80 lb +  FX = 0.4 (80) – P = 0 P = lb P B A N F=0.4 N 30 lb 50 lb

60 GROUP PROBLEM SOLVING (continued)
 +  Fy = N cos 20 N sin 20 – 30 = N = lb  +  Fx = – P ( 26.2 ) cos 20 – 26.2 sin 20 = P = lb 20º 30 lb 0.6 N P N Case b (block B slides over A): Case b has the lowest P (case a was 32 lb) and thus will occur first. Next, using a frictional force analysis of belt, we get WD = P e   = e 0.5 ( 0.5  ) = lb A Block D weighing 12.7 lb will cause the block B to slide over the block A.

61 A) The wedge B) The block
ATTENTION QUIZ 1. When determining the force P needed to lift the block of weight W, it is easier to draw a FBD of ______ first. A) The wedge B) The block C) The horizontal ground D) The vertical wall W 2. In the analysis of frictional forces on a flat belt, T2 = T1 e  . In this equation,  equals ______ . A) Angle of contact in degrees B) Angle of contact in radians C) Coefficient of static friction D) Coefficient of kinetic friction Answers: 1.A 2.B Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5

62 End of the Lecture Let Learning Continue
In the last slide add the ‘home’ action button Statics:The Next Generation (2nd Ed.) Mehta, Danielson, & Berg Lecture Notes for Sections 8.3,8.5


Download ppt "CHARACTERISTICS OF DRY FRICTION & PROBLEMS INVOLVING DRY FRICTION"

Similar presentations


Ads by Google