SOLUTION

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8–7.

The block brake consists of a pin-connected lever and friction block at B . The coefficient of static friction between the wheel and the lever is m s

=

0.3, and a torque of 5 N

# m is applied to the wheel. Determine if the brake can hold the wheel stationary when the force applied to the lever is

(a) P = 30 N, (b) P = 70 N.

SOLUTION

To hold lever: a + © M

O

=

0;

F

B

(0.15)

-

5

=

0;

Require

F

B

=

33.333 N

N

B

=

33.333 N

0.3

= 111.1 N

Lever,

P

Reqd.

(0.6) 111.1(0.2) 33.333(0.05) = 0 a + © M

A

= 0;

P

Reqd.

b)

= 39.8 N a) P = 30 N 6 39.8 N No

P = 70 N 7 39.8 N Yes

5 N m

50 mm

A

150 mm

O

B

200 mm 400 mm

P

A n s .

A n s .

*8–8.

The block brake consists of a pin-connected lever and friction block at B . The coefficient of static friction between the wheel and the lever is m s

=

0.3

, and a torque of 5 N

# m is applied to the wheel. Determine if the brake can hold the wheel stationary when the force applied to the lever is

(a) P = 30 N , (b) .

SOLUTION

To hold lever: a + © M

O

= 0; F

B

(0.15) + 5 = 0;

Require

N

B

=

33.333 N

0.3

= 111.1 N

F

B

= 33.333 N

Lever,

P

Reqd.

(0.6) 111.1(0.2) + 33.333(0.05) = 0 a + © M

A

= 0;

P

Reqd.

= 34.26 N a) P = 30 N 6 34.26 N No b) P = 70 N 7 34.26 N Yes

5 N m

50 mm

A

150 mm

O

B

200 mm 400 mm

P

A n s .

A n s .

8–23.

A 35-kg disk rests on an inclined surface for which m s

=

0.2.

Determine the maximum vertical force P that may be applied to link AB without causing the disk to slip at C .

200 mm

300 mm

P

600 mm

SOLUTION

Equations of Equilibrium: From FBD (a), a + © M

B

=

0;

P 1

600

2 A y

1

900

2 =

0

From FBD (b),

+ c © F y

= 0 a + © M

O

= 0;

A y

=

0.6667

P

N

C sin 60° F

C sin 30° 0.6667

P 343.35

= 0

F

C

1 200 2 0.6667

P 1 200 2 = 0

(1)

(2)

Friction: If the disk is on the verge of moving, slipping would have to occur at point C . Hence, F

C

= m s

N

C

= 0.2

N

C

.

Substituting this value into Eqs. (1) and (2) and solving, we have

P =

182 N

N

C

=

606.60 N

A n s .

C

200 mm

A

30

°

B

8–46.

The beam AB has a negligible mass and thickness and is subjected to a triangular distributed loading. It is supported at one end by a pin and at the other end by a post having a mass of 50 kg and negligible thickness. Determine the minimum force P needed to move the post. The coefficients of static friction at B and C m

B

= 0.4

= 0.2, respectively.

SOLUTION

Member AB: a + © M

A

= 0; 800 a

4

3 b + N

B

(2) = 0

N

B

= 533.3 N

Post:

Assume slipping occurs at C ; F

C

= 0.2

N

C a + © M

C

= 0; -

4

5

P (0.3) + F

B

(0.7) = 0

F x

= 0;

4

5

P F

B

0.2

N

C

= 0

+ c © F y

= 0;

3

5

P + N

C

533.3

50(9.81) = 0

P = 355 N

N

C

= 811.0 N

F

B

= 121.6 N

( F

B

) max

= 0.4(533.3) = 213.3 N 7 121.6 N

A

A n s .

(O.K.

!

)

2 m

400 mm

800 N

/ m

B

5

4

3

P

300 mm

C

8–47.

The beam AB has a negligible mass and thickness and is subjected to a triangular distributed loading. It is supported at one end by a pin and at the other end by a post having a mass of 50 kg and negligible thickness. Determine the two coefficients of static friction at B and at C so that when the magnitude of the applied force is increased to P = 150 N, the post slips at both B and C simultaneously.

SOLUTION

Member AB: a + © M

A

= 0; 800 a

4

3 b + N

B

(2) = 0

N

B

= 533.3 N

Post:

+ c © F y

= 0; N

C

533.3

+ 150 a

3

5 b - 50(9.81) = 0

N

C

= 933.83 N a + © M

C

= 0; -

4

5

(150)(0.3) + F

B

(0.7) = 0

F

B

= 51.429 N

+ ©

F x

= 0;

4

5

(150) F

C

51.429

= 0

F

C

=

68.571 N m

C

=

F

C

N

C

=

68.571

933.83

= 0.0734

m

B

=

F

B

N

B

=

51.429

533.3

= 0.0964

A

A n s .

A n s .

2 m

400 mm

800 N

/ m

B

5

4

3

P

300 mm

C

8–65.

The coefficient of static friction between wedges B and C is m

C s

= 0.6

and D , and between the surfaces of contact m s

¿ =

0.4.

B and A and

If the spring is compressed 200 mm when in the position shown, determine the smallest force P needed to move wedge C to the left. Neglect the weight of the wedges.

SOLUTION

Wedge B :

: F x

=

0;

+ c © F y

=

0;

N

AB

-

0.6

N

BC cos 15°

N

BC

sin 15°

=

0

N

BC cos 15°

-

0.6

N

BC sin 15°

-

0.4

N

AB

-

100

=

0

N

BC

=

210.4 N

N

AB

=

176.4 N

Wedge C :

+ c © F y

= 0;

+ ©

F x

= 0;

N

CD cos 15° 0.4

N

CD sin 15° + 0.6(210.4) sin 15° 210.4 cos 15° = 0

N

CD

= 197.8 N

197.8 sin 15° + 0.4(197.8) cos 15° + 210.4 sin 15° + 0.6(210.4) cos 15° P = 0

P = 304 N A n s .

k 500 N

/ m

A

15

B

D

15

15

C P

8–66.

The coefficient of static friction between the wedges B and

C is and m

C s

= and

0.6

D , and between the surfaces of contact m s

¿ =

0.4.

If

P =

50 N,

B and A determine the largest allowable compressionof the spring without causing wedge C to move to the left. Neglect the weight of the wedges.

SOLUTION

Wedge C :

+ ©

F x

= 0; c + © F y

= 0;

( N

CD

+ N

BC

) sin 15° + (0.4

N

CD

+ 0.6

N

BC

) cos 15° 50 = 0

( N

CD

N

BC

) cos 15° + ( 0.4

N

CD

+ 0.6

N

BC

) sin 15° = 0

N

BC

= 34.61 N

N

CD

= 32.53 N

Wedge B :

: F x

=

0; c + © F y

=

0;

N

AB

-

0.6(34.61) cos 15°

-

34.61 sin 15°

=

0

N

AB

=

29.01 N

34.61 cos 15°

-

0.6(34.61) sin 15°

-

0.4(29.01)

-

500 x =

0 x =

0.03290 m

=

32.9 mm A n s .

k 500 N / m

A

15

B

D

15

15

C P

*8–92.

The s imple band brake i s con s tructed s o that the end s of the friction s trap are connected to the pin at A and the le v er arm

# at B . If the wheel i s s ubjected to a torque of M

=

80 lb ft, and the minimum force P = 20 lb i s needed to apply to the le v er to hold the wheel s tationary, determine the coefficient of s tatic friction between the wheel and the band.

SOLUTION

Eq u at i ons of Eq ui l i br iu m : Write the moment equation of equilibrium about point A by referrin g to the FBD of the le v er s hown in Fi g .

a , a

+ ©

M

A =

0 ; T

B s in 45°(1 .5)

-

20(4 .5)

=

0 T

B =

84 .85 lb

U s in g thi s re s ult to write the moment equation of equilibrium about point 0 by referrin g to the FBD of the wheel s hown in Fi g .

b , a

+ ©

M

O =

0 ; T

A

(1 .25)

+

80

-

84 .85(1 .25)

=

0 T

A =

20 .85 lb

Fr i ct i onal Force on Flat Belt : Here, b

= a

245°

180° b p

=

T

2

= T

B

= 84.85 lb. Applyin g Eq. 8–6,

T

2

=

T

1 e mb

84 .85

=

20 .85

e m (

49

36

) p e m (

49

36

) p

=

4 .069

In e m (

49

36

) p

=

In 4 .069

49

36 p , T

1 =

T

A =

20 .85 lb and m a

49

36 b p

=

In 4 .069

m

=

0 .328

Ans.

20 ⬚

M

80 lb

ft

O

45

1.25 ft

A

B

1.5 ft 3 ft

P

8–93.

The simple band brake is constructed so that the ends of the friction strap are connected to the pin at A and the lever arm at B

M = 80 lb

# . If the wheel is subjected to a torque of ft, determine the smallest force P applied to the lever that is required to hold the wheel stationary. The coefficient of static friction between the strap and wheel is m s

=

0.5.

SOLUTION b =

20°

+

180°

+

45°

=

245° a + © M

O

=

0;

T

2

= T

1 e mb

;

T

1

(1.25)

+

80

T

2

(1.25)

=

0

T

2

= T

1 e 0.5(245°)( p

180°

) =

8.4827

T

1

Solving;

T

1

= 8.553 lb

T

2

= 72.553 lb a + © M

A

= 0;

P = 17.1 lb

72.553(sin 45°)(1.5) 4.5

P = 0

A n s .

20

M 80 lb ft

O

45

1.25 ft

A

B

1.5 ft 3 ft

P

8–130.

The hand cart has wheels with a diameter of 80 mm. If a crate having a mass of 500 kg is placed on the cart so that each wheel carries an equal load, determine the horizontal force P that must be applied to the handle to overcome the rolling resistance. The coefficient of rolling resistance is

2 mm. Neglect the mass of the cart.

SOLUTION

P L

Wa r

= 500 1 9.81

2a

2

40 b

P =

245 N A n s .

P

8–141.

The jacking mechanism consists of a link that has a squarethreaded screw with a mean diameter of 0.5 in. and a lead of

0.20 in., and the coefficient of static friction is m s

=

0.4

.

Determine the torque M that should be applied to the screw to start lifting the 6000-lb load acting at the end of member ABC .

SOLUTION

A a = tan

1 a

10

25 b = 21.80° a + © M

A

= 0; 6000 (35) + F

BD

cos 21.80° (10) + F

BD

sin 21.80° (20) = 0

F

BD

= 12 565 lb f s

= tan

1 (0.4) = 21.80° u = tan

1 a

0.2

2 p (0.25) b = 7.256°

M = Wr tan ( u + f )

M = 12 565 (0.25) tan (7.256° + 21.80°)

M = 1745 lb

# in = 145 lb

# ft A n s .

20 in.

B

15 in.

M

6000 lb

C

10 in.

7.5 in.

10 in.

D

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