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Solucionário - Projeto de Máquinas 4 Ed., Exercícios de Engenharia Mecânica

Livro solucionário Projeto de Maquinas (Norton).

Tipologia: Exercícios

2021

Compartilhado em 27/01/2021

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MACHINE DESIGN - An Integrated Approach, 4th Ed. 1-1-1
PROBLEM 1-1
Statement: It is often said, "Build a better mousetrap and the world will beat a path to your door." Consider
this problem and write a goal statement and a set of at least 12 task specifications that you would
apply to its solution. Then suggest 3 possible concepts to achieve the goal. Make annotated,
freehand sketches of the concepts.
Solution:
Goal Statement: Create a mouse-free environment.
Task Specifications:
1. Cost less than $1.00 per use or application.
2. Allow disposal without human contact with mouse.
3. Be safe for other animals such as house pets.
4. Provide no threat to children or adults in normal use.
5. Be a humane method for the mouse.
6. Be environmentally friendly.
7. Have a shelf-life of at least 3 months.
8. Leave no residue.
9. Create minimum audible noise in use.
10. Create no detectable odors within 1 day of use.
11. Be biodegradable.
12. Be simple to use with minimal written instructions necessary.
Concepts and sketches are left to the student. There are an infinity of possibilities.
P0101.xmcd
© 2011 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This publication is protected by Copyright and written permission should be
obtained from the publisher prior to any prohibited reproduction, storage in a retrieval system, or transmission in any form or by any means, electronic,
mechanical, photocopying, recording, or likewise. For information regarding permission(s), write to: Rights and Permissions Department,
Pearson Education, Inc., Upper Saddle River, NJ 07458.
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Baixe Solucionário - Projeto de Máquinas 4 Ed. e outras Exercícios em PDF para Engenharia Mecânica, somente na Docsity!

PROBLEM 1-

Statement: It is often said, "Build a better mousetrap and the world will beat a path to your door." Consider this problem and write a goal statement and a set of at least 12 task specifications that you would apply to its solution. Then suggest 3 possible concepts to achieve the goal. Make annotated, freehand sketches of the concepts.

Solution:

Goal Statement: Create a mouse-free environment. Task Specifications:

  1. Cost less than $1.00 per use or application.
  2. Allow disposal without human contact with mouse.
  3. Be safe for other animals such as house pets.
  4. Provide no threat to children or adults in normal use.
  5. Be a humane method for the mouse.
  6. Be environmentally friendly.
  7. Have a shelf-life of at least 3 months.
  8. Leave no residue.
  9. Create minimum audible noise in use.
  10. Create no detectable odors within 1 day of use.
  11. Be biodegradable.
  12. Be simple to use with minimal written instructions necessary. Concepts and sketches are left to the student. There are an infinity of possibilities.

PROBLEM 1-

Statement: A bowling machine is desired to allow quadriplegic youths, who can only move a joystick, to engage in the sport of bowling at a conventional bowling alley. Consider the factors involved, write a goal statement, and develop a set of at least 12 task specifications that constrain this problem. Then suggest 3 possible concepts to achieve the goal. Make annotated, freehand sketches of the concepts.

Solution:

Goal Statement: Create a means to allow a quadriplegic to bowl. Task Specifications:

  1. Cost no more than $2 000.
  2. Portable by no more than two able-bodied adults.
  3. Fit through a standard doorway.
  4. Provide no threat of injury to user in normal use.
  5. Operate from a 110 V, 60 Hz, 20 amp circuit.
  6. Be visually unthreatening.
  7. Be easily positioned at bowling alley.
  8. Have ball-aiming ability, controllable by user.
  9. Automatically reload returned balls.
  10. Require no more than 1 able-bodied adult for assistance in use.
  11. Ball release requires no more than a mouth stick-switch closure.
  12. Be simple to use with minimal written instructions necessary. Concepts and sketches are left to the student. There are an infinity of possibilities.

PROBLEM 1-

Statement: Convert a mass of 1 000 lbm to (a) lbf, (b) slugs, (c) blobs, (d) kg.

Units: blob lbf sec

^2

in

Given: Mass M := 1000  lb

Solution: See Mathcad file P0104.

  1. To determine the weight of the given mass, multiply the mass value by the acceleration due to gravity, g.

W := M gW = 1000 lbf

  1. Convert mass units by assigning different units to the units place-holder when displaying the mass value.

Slugs (^) M =31.081 slug Blobs (^) M =2.59 blob Kilograms (^) M =453.592 kg

PROBLEM 1-

Statement: A 250-lbm mass is accelerated at 40 in/sec2. Find the force in lb needed for this acceleration.

Given: Mass M := 250  lb Acceleration a 40 in sec^2

Solution: See Mathcad file P0105.

  1. To determine the force required, multiply the mass value, in slugs, by the acceleration in feet per second squared.

Convert mass to slugs: (^) M =7.770 slug Convert acceleration to feet per second squared: (^) a =3.333 s -^2  ft F := M aF =25.9 lbf

PROBLEM 1-

Statement: Prepare an interactive computer program (using, for example, Excell, Mathcad, or TKSolver) from which the cross-sectional properties for the shapes shown in the inside front cover can be calculated. Arrange the program to deal with both ips and SI unit systems and convert the results between those systems.

Solution: See the inside front cover and Mathcad file P0107.

  1. Rectangle, let: b  3  in h  4  in Area (^) A  b hA 12.000  in^2 A  7742  mm^2

Moment about x -axis (^) Ix b h

^3

 12 Ix 16.000 in  ^4 Ix 6.660  106  mm^4

Moment about y -axis (^) Iy h b

^3

 12 Iy 9.000 in  ^4 Iy 3.746  106  mm^4

Radius of gyration about x -axis (^) k (^) x Ix  (^) A k (^) x 1.155  in k (^) x 29.329  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) A k (^) y 0.866  in k (^) y 21.997  mm

Polar moment of inertia (^) J (^) z  IxIy J (^) z 25.000  in^4 J (^) z 1.041  107  mm^4

  1. Solid circle, let: D  3  in Area (^) A^ π^ D

^2

 4 A 7.069 in  ^2 A  4560  mm^2

Moment about x -axis (^) Ix^ π^ D

^4

 64 Ix 3.976 in  ^4 Ix 1.655  106  mm^4

Moment about y -axis (^) Iy^ π^ D

^4

 64 Iy 3.976 in  ^4 Iy 1.655  106  mm^4

Radius of gyration about x -axis (^) k (^) x Ix  (^) A k (^) x 0.750  in k (^) x 19.05  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) A k k (^) y (^) y 0.75019.05   inmm

Polar moment of inertia (^) J (^) z^ π^ D

^4

 32 J (^) z 7.952 in  ^4 J (^) z 3.310  106  mm^4

  1. Hollow circle, let:

D  3  in d  1  in Area (^) A^ π 4 D

 ^2  d^2  A 6.283  in^2

A  4054  mm^2

Moment about x -axis (^) Ix^ π 64 D

 ^4  d^4  Ix 3.927  in^4

Ix 1.635  106  mm^4

Moment about y -axis (^) Iy^ π 64 D

 ^4  d^4  Iy 3.927  in^4

Iy 1.635  106  mm^4

Radius of gyration about x -axis (^) k (^) x Ix  (^) A k (^) x 0.791  in k (^) x 20.08  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) A k (^) y 0.791  in k (^) y 20.08  mm

Polar moment of inertia (^) J (^) z^ π 32 D

 ^4  d^4  J z 7.854  in^4

J (^) z 3.269  106  mm^4

  1. Solid semicircle, let:

D  3  in R  0.5  D R 1.5 in

Area (^) A^ π^ D

^2

 8 A 3.534 in  ^2 A  2280  mm^2

Moment about x -axis (^) Ix  0.1098  R^4 Ix 0.556  in^4 Ix 2.314  105  mm^4 Moment about y -axis (^) Iy^ π^ R

^4

 8 Iy 1.988 in  ^4 Iy 8.275  105  mm^4

PROBLEM 1-

Statement: Prepare an interactive computer program (using, for example, Excell, Mathcad, or TKSolver) from which the mass properties for the solids shown in the page opposite the inside front cover can be calculated. Arrange the program to deal with both ips and SI unit systems and convert the results between those systems.

Units: blob lbf sec

^2

 in

Solution: See the page opposite the inside front cover and Mathcad file P0108.

  1. Rectangular prism, let: a  2  in b  3  in c  4  in γ 0.28  lbfin ^3

Volume (^) V  a b   c V 24.000  in^3 V  393290  mm^3 Mass (^) M V ^ γ  (^) g M 0.017  blob M 3.048  kg

Moment about x -axis (^) Ix M^ a

^2  b^2 

 12 Ix 0.019 blob in   ^2 Ix 2130.4  kg mm ^2

Moment about y -axis (^) Iy M^ a

^2  c^2 

 12 Iy 0.029 blob in   ^2 Iy 3277.6  kg mm ^2

Moment about z -axis (^) Iz M^ b

^2  c^2 

 12 Iz 0.036 blob in   ^2 Iz 4097.0  kg mm ^2

Radius of gyration about x -axis (^) k (^) x Ix  (^) M k (^) x 1.041  in k (^) x 26.437  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) M k (^) y 1.291  in k (^) y 32.791  mm

Radius of gyration about z -axis (^) k (^) z Iz  (^) M k (^) z 1.443  in k (^) z 36.662  mm

2.Cylinder, let: r  2  in L  3  in γ 0.30  lbfin ^3

Volume (^) V  π  r 2  L V 37.699  in^3 V  617778  mm^3 Mass (^) M V ^ γ  (^) g M 0.029  blob M 5.13  kg

Moment about x -axis (^) Ix M r

^2

 2 Ix 0.059 blob in   ^2 Ix 6619.4  kg mm ^2 Moment about y -axis (^) Iy M^^3 r

^  2  L^2 

 12 Iy 0.051 blob in   ^2 Iy 5791.9  kg mm ^2 Moment about z -axis (^) Iz M^^3 r

^  2  L^2 

 12 Iz 0.051 blob in   ^2 Iz 5791.9  kg mm ^2

Radius of gyration about x -axis (^) k (^) x Ix  (^) M k (^) x 1.414  in k (^) x 35.921  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) M k (^) y 1.323  in k (^) y 33.601  mm

Radius of gyration about z -axis (^) k (^) z Iz  (^) M k (^) z 1.323  in k (^) z 33.601  mm

  1. Hollow cylinder, let:

a  2  in b  3  in L  4  in γ 0.28  lbfin ^3

Volume V  π  b^2  a^2  L V 62.832  in^3

V  1029630  mm^3

Mass (^) M V ^ γ  (^) g M 0.046  blob M 7.98  kg

Moment about x -axis (^) Ix M 2 a

 ^2  b^2  Ix 0.296  blob in ^2

Ix 3.3  104  kg mm ^2

Moment about y -axis (^) Iy M 12 3 a

 ^  2  3  b^2  L^2  Iy 0.209  blob in ^2

Iy 2.4  104  kg mm ^2

Moment about z -axis (^) Iz M 12 3 a

 ^  2  3  b^2  L^2  Iz 0.209  blob in ^2

Iz 2.4  104  kg mm ^2

Radius of gyration about x -axis (^) k (^) x Ix  (^) M k (^) x 2.550  in k (^) x 64.758  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) M k (^) y 2.141  in k (^) y 54.378  mm

Moment about y -axis (^) Iy^2 5 ^ Mr  ^2 Iy 0.295  blob in ^2 Iy  33362  kg mm ^2

Moment about z -axis (^) Iz^2 5 ^ Mr  ^2 Iz 0.295  blob in ^2 Iz  33362  kg mm ^2

Radius of gyration about x -axis (^) k (^) x Ix  (^) M k (^) x 1.897  in k (^) x 48.193  mm

Radius of gyration about y -axis (^) k (^) y Iy  (^) M k (^) y 1.897  in k (^) y 48.193  mm

Radius of gyration about z -axis (^) k (^) z Iz  (^) M k (^) z 1.897  in k (^) z 48.193  mm

PROBLEM 1-

Statement: Convert the template in Problem 1-7 to have and use a set of functions or subroutines that can be called from within any program in that language to solve for the cross-sectional properties of the shapes shown on the inside front cover.

Solution: See inside front cover and Mathcad file P0109.

  1. Rectangle: Area (^) A b h ( )  b h

Moment about x -axis (^) Ix ( b h ) b h

^3

Moment about y -axis (^) Iy ( b h ) h b

^3

  1. Solid circle: Area (^) A D ( )^ π^ D

^2

Moment about x -axis (^) Ix ( D )^ π^ D

^4

Moment about y -axis (^) Iy ( D )^ π^ D

^4

  1. Hollow circle: Area (^) A D d ( )^ π 4 D

 ^2  d^2 

Moment about x -axis (^) Ix ( D d )^ π 64 D

 ^4  d^4 

Moment about y -axis (^) Iy ( D d )^ π 64 D

 ^4  d^4 

  1. Solid semicircle: Area (^) A D ( )^ π^ D

^2

Moment about x -axis (^) Ix ( R ) 0.1098  R^4

Moment about y -axis (^) Iy ( R )^ π^ R

^4

  1. Right triangle: Area (^) A b h ( ) b h   2

Moment about x -axis (^) Ix ( b h ) b h

^3

Moment about y -axis (^) Iy ( b h ) h b

^3

  1. Right circular cone:

Volume (^) V r h ( )^ π^ r  2  h  3

Mass (^) M r h (  γ) V r h (^ )^ γ  g

Moment about x -axis (^) Ix ( r h  γ) 3 10 ^ M r h (^ ^ γ) r

 ^2

Moment about y -axis (^) Iy ( r h  γ) M r h (  γ) 12 r

  2  3  h^2 

Moment about z -axis (^) Iz ( r h  γ) M r h (  γ) 12 r

  2  3  h^2 

  1. Sphere:

Volume (^) V r ( ) 4 3 ^ π r

 ^3

Mass (^) M r (  γ) V r ( )^ γ  g

Moment about x -axis (^) Ix ( r  γ) 2 5 ^ M r (^ ^ γ) r

 ^2

Moment about y -axis (^) Iy ( r  γ) 2 5 ^ M r (^ ^ γ) r

 ^2

Moment about z -axis (^) Iz ( r  γ) 2 5 ^ M r (^ ^ γ) r

 ^2

PROBLEM 2-

Statement: Figure P2-1 shows stress-strain curves for three failed tensile-test specimens. All are plotted on the same scale. (a) Characterize each material as brittle or ductile. (b) Which is the stiffest? (c) Which has the highest ultimate strength? (d) Which has the largest modulus of resilience? (e) Which has the largest modulus of toughness?

Solution: See Figure P2-1 and Mathcad file P0201.

  1. The material in Figure P2-1(a) has a moderate amount of strain beyond the yield point, P2-1(b) has very little, and P2-1(c) has considerably more than either of the other two. Based on this observation, the material in Figure P2-1(a) is mildly ductile , that in P2-1(b)is brittle , and that in P2-1(c) is ductile.
  2. The stiffest material is the one with the grearesr slope in the elastic range. Determine this by dividing the rise by the run of the straight-line portion of each curve. The material in Figure P2-1(c) has a slope of 5 stress units per strain unit, which is the greatest of the three. Therefore, P2-1(c) is the stiffest.
  3. Ultimate strength corresponds to the highest stress that is achieved by a material under test. The material in Figure P2-1(b) has a maximum stress of 10 units, which is considerably more than either of the other two. Therefore, P2-1(b) has the highest ultimate strength.
  4. The modulus of resilience is the area under the elastic portion of the stress-starin curve. From observation of the three graphs, the stress and strain values at the yield points are: P2-1(a) σ ya := 5 ε ya := 5 P2-1(b) σ yb := 9 ε yb := 2 P2-1(c) σ yc := 5 ε yc := 1 Using equation (2.7), the modulus of resiliency for each material is, approximately,

P21a := 12 ⋅ σ ya ⋅ ε ya P21a =12.

P21b := 12 ⋅ σ yb ⋅ ε yb P21b = 9

P21c := 12 ⋅ σ yc ⋅ ε yc P21c =2.

P2-1 (a) has the largest modulus of resilience

  1. The modulus of toughness is the area under the stress-starin curve up to the point of fracture. By inspection, P2-1 (c) has the largest area under the stress-strain curve therefore, it has the largest modulus of toughness.

PROBLEM 2-

Statement: Which of the steel alloys shown in Figure 2-19 would you choose to obtain (a) Maximum strength (b) Maximum modulus of resilience (c) Maximum modulus of toughness (d) Maximum stiffness

Given: Young's modulus for steel E  207  GPa Solution: See Figure 2-19 and Mathcad file P0203.

  1. Determine from the graph: values for yield strength, ultimate strength and strain at fracture for each material.

Steel Yield Strength Ultimate Strength Fracture Strain AISI 1020: (^) Sy 1020  300  MPa Sut 1020  400  MPa ε f 1020 0. AISI 1095: (^) Sy 1095  550  MPa Sut 1095  1050  MPa ε f 1095 0. AISI 4142: (^) Sy 4142  1600  MPa Sut 4142  2430  MPa ε f 4142 0. Note: The 0.2% offset method was used to define a yield strength for the AISI 1095 and the 4142 steels.

  1. From the values of Sut above it is clear that the AISI 4142 has maximum strength.
  2. Using equation (2-7) and the data above, determine the modulus of resilience.

UR1020^12 Sy 1020^2   E UR1020 0. MN mm^3

UR1095^12

Sy 1095^2   E UR1095 0. MN mm^3

UR4142^12

Sy 4142^2   E UR4142 6. MN mm^3

Even though the data is approximate, the AISI 4142 clearly has the largest modulus of resilience.

  1. Using equation (2-8) and the data above, determine the modulus of toughness.

UT1020  12  Sy (^) 1020Sut 1020  ε f 1020 UT1020 128 MN mm^3

UT1095  12  Sy (^) 1095Sut 1095  ε f 1095 UT1095 88 MN mm^3

UT4142  12  Sy (^) 4142Sut 4142  ε f 4142 UT4142 121 MN mm^3

Since the data is approximate, there is no significant difference between the 1020 and 4142 steels. Because of the wide difference in shape and character of the curves, one should also determine the area under the curves by graphical means. When this is done, the area under the curve is about 62 square units for 1020 and 66 for 4142. Thus, they seem to have about equal toughness, which is about 50% greater than that for the 1095 steel.

  1. All three materials are steel therefore, the stiffnesses are the same.

PROBLEM 2-

Statement: Which of the aluminum alloys shown in Figure 2-21 would you choose to obtain (a) Maximum strength (b) Maximum modulus of resilience (c) Maximum modulus of toughness (d) Maximum stiffness

Given: Young's modulus for aluminum E 71.7  GPa Solution: See Figure 2-21 and Mathcad file P0204.

  1. Determine, from the graph, values for yield strength, ultimate strength and strain at fracture for each material.

Alum Yield Strength Ultimate Strength Fracture Strain 1100: (^) Sy 1100  120  MPa Sut 1100  130  MPa ε f 1100 0. 2024-T351: (^) Sy 2024  330  MPa Sut 2024  480  MPa ε f 2024 0. 7075-T6: (^) Sy 7075  510  MPa Sut 7075  560  MPa ε f 7075 0. Note: The 0.2% offset method was used to define a yield strength for all of the aluminums.

  1. From the values of Sut above it is clear that the 7075-T6 has maximum strength.
  2. Using equation (2-7) and the data above, determine the modulus of resilience.

UR1100^12 Sy 1100^2   E UR1100 0. MN mm^3

UR2024^12

Sy 2024^2   E UR2024 0. MN mm^3

UR7075^12

Sy 7075^2   E UR7075 1. MN mm^3

Even though the data is approximate, the 7075-T6 clearly has the largest modulus of resilience.

  1. Using equation (2-8) and the data above, determine the modulus of toughness.

UT1100  12  Sy (^) 1100Sut 1100  ε f 1100 UT1100 21 MN mm^3

UT2024  12  Sy (^) 2024Sut 2024  ε f 2024 UT2024 79 MN mm^3

UT7075  12  Sy (^) 7075Sut 7075  ε f 7075 UT7075 88 MN mm^3

Even though the data is approximate, the 7075-T6 has the largest modulus of toughness.

  1. All three materials are aluminum therefore, the stiffnesses are the same.