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    751

    Consider the equilibrium of the FBD of the top cut segment in Fig.a,

    a

    The normal stress developed is the combination of axial and bending stress.Thus,

    For the left edge fiber, . Then

    Ans.

    For the right edge fiber, . Then

    Ans.sR = - 100 (103)

    0.006 +

    10(103)(0.1)

    20.0(10- 6)= 33.3 MPa (T)

    y = 0.1 m

    = -66.67(106) Pa = 66.7 MPa (C)

    sL = -100(103)

    0.006 -

    10(103)(0.1)

    20.0(10- 6)

    y = C = 0.1 m

    s =N

    A ;

    My

    I

    A = 0.2(0.03) = 0.006 m2I =1

    12(0.03)(0.23) = 20.0(10- 6) m4

    + MC = 0;100(0.1) - M = 0M = 10 kN # m

    + c Fy = 0;N - 100 = 0N = 100 kN

    819. Determine the maximum and minimum normalstress in the bracket at section aa when the load is appliedat .x = 0

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    100 kN

    x

    200 mm150 mm

    15 mm

    15 mm

    aa

    Ans:

    sL = 66.7 MPa (C), sR = 33.3 MPa (T)

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    752

    Consider the equilibrium of the FBD of the top cut segment in Fig.a,

    a

    The normal stress developed is the combination of axial and bending stress.Thus,

    For the left edge fiber, . Then

    Ans.

    For the right edge fiber, . Thus

    Ans.= 117 MPa (C)

    sR = -100(103)

    0.006 -

    20.0(103)(0.1)

    20.0(10- 6)

    y = C = 0.1 m

    = 83.33(106) Pa = 83.3 MPa (T)

    sR = -100(103)

    0.006 +

    20.0(103)(0.1)

    20.0(10- 6)

    y = C = 0.1 m

    s =

    N

    A ;

    My

    I

    A = 0.2 (0.03) = 0.006 m2I =1

    12(0.03)(0.23) = 20.0(10- 6) m4

    + MC = 0;M - 100(0.2) = 0M = 20 kN # m

    + c Fy = 0;N - 100 = 0N = 100 kN

    *820. Determine the maximum and minimum normalstress in the bracket at section aa when the load is appliedat x = 300 mm.

    100 kN

    x

    200 mm150 mm

    15 mm

    15 mm

    aa

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

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    758

    Section Properties: The location of the centroid of the cross section, Fig.a, is

    The cross - sectional area and the moment of inertia about the z axis of the crosssection are

    = 1.5609(10- 3) m4

    Iz =1

    12(0.3)(0.153) + 0.3(0.15)(0.1875 - 0.075)2 +

    1

    12(0.15)(0.33) + 0.15(0.3)(0.3 - 0.1875)2

    A = 0.15(0.3) + 0.3(0.15) = 0.09 m2

    y = yA

    A =

    0.075(0.15)(0.3) + 0.3(0.3)(0.15)

    0.15(0.3) + 0.3(0.15) = 0.1875 m

    826. The column is built up by gluing the two identicalboards together. Determine the maximum normal stressdeveloped on the cross section when the eccentric force of

    is applied.P = 50 kN

    150 mm

    150 mm

    250 mm

    75 mm

    300 mm

    50 mm

    P

    Equivalent Force System: Referring to Fig. b,

    Normal Stress: The normal stress is a combination of axial and bending stress. Thus,

    By inspection, the maximum normal stress occurs at points along the edge wheresuch as point A. Thus,

    Ans.= -2.342 MPa = 2.34 MPa (C)

    smax = -50(103)

    0.09 -

    10.625(103)(0.2625)

    1.5609(10 - 3)

    y = 0.45 - 0.1875 = 0.2625 m

    s =N

    A +My

    I

    M = 10.625 kN # m-50(0.2125) = -MMz = (MR)z;

    F = 50 kN-50 = -F+ c Fx = (FR)x;

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    Ans:

    smax = 2.34 MPa (C)

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    759

    827. The column is built up by gluing the two identicalboards together. If the wood has an allowable normal stressof , determine the maximum allowableeccentric force P that can be applied to the column.

    sallow = 6 MPa

    Section Properties: The location of the centroid c of the cross section, Fig.a, is

    The cross-sectional area and the moment of inertia about the z axis of the crosssection are

    A = 0.15(0.3) + 0.3(0.15) = 0.09 m2

    y = yA

    A =

    0.075(0.15)(0.3) + 0.3(0.3)(0.15)

    0.15(0.3) + 0.3(0.15) = 0.1875 m

    150 mm

    150 mm

    250 mm

    75 mm

    300 mm

    50 mm

    P

    = 1.5609(10 - 3) m4

    Iz =1

    12(0.3)(0.153) + 0.3(0.15)(0.1875 - 0.075)2 +

    1

    12(0.15)(0.33) + 0.15(0.3)(0.3 - 0.1875)2

    Equivalent Force System: Referring to Fig.b,

    Normal Stress: The normal stress is a combination of axial and bending stress. Thus,

    By inspection, the maximum normal stress, Which is compression, occurs at pointsalong the edge where such as point A.Thus,

    Ans.P = 128 076.92 N = 128 kN

    -6(106) = -P

    0.09 -

    0.2125P(0.2625)

    1.5609(10- 3)

    y = 0.45 - 0.1875 = 0.2625 m

    F =N

    A +My

    I

    M = 0.2125P-P(0.2125) = -MMz = (MR)z;

    F = P-P = -F+c Fx = (FR)x;

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    Ans:

    P = 128 kN

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    773

    838. The frame supports the distributed load shown.Determine the state of stress acting at point D. Show theresults on a differential element at this point.

    Ans.

    Ans.tD = 0

    sD = - 88.0 MPa

    sD = -P

    A -

    My

    I = -

    8(103)

    (0.1)(0.05) -

    12(103)(0.03)112 (0.05)(0.1)

    3

    4 kN/m

    D

    B

    A

    C

    E

    1.5 m 1.5 m

    20 mm

    50 mm

    20 mm

    60 mm

    3 m

    3 m

    5 m

    D

    E

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    Ans:

    sD = - 88.0 MPa, tD = 0

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    774

    Ans.

    Ans.tE = VQ

    It =

    4.5(103)(0.04)(0.02)(0.05)1

    12 (0.05)(0.1)3(0.05)

    = 864 kPa

    sE = -P

    A -My

    I =

    8(103)

    (0.1)(0.05) +

    8.25(103)(0.03)1

    12(0.05)(0.1)3

    = 57.8 MPa

    839. The frame supports the distributed load shown.Determine the state of stress acting at point E. Show theresults on a differential element at this point.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    4 kN/m

    D

    B

    A

    C

    E

    1.5 m 1.5 m

    20 mm

    50 mm

    20 mm

    60 mm

    3 m

    3 m

    5 m

    D

    E

    Ans:

    sE = 57.8 MPa, tE = 864 kPa

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    775

    Support Reactions: Referring to the free-body diagram of the entire boom, Fig.a,

    Internal Loadings: Considering the equilibrium of the free-body diagram of the boomsright cut segment,Fig.b,

    Section Properties: The cross-sectional area and the moment of inertia about thecentroidal axis of the booms cross section are

    Referring to Fig. c, QA is

    Normal Stress: The normal stress is the combination of axial and bending stress.Thus,

    For point Then

    Ans.

    Shear Stress: The shear stress is contributed by transverse shear stress only.Thus,

    Ans.

    The state of stress at pointA is represented on the element shown in Fig. d.

    tA = VQA

    It =

    1465.75[0.589(10- 3)]

    0.14709(10 - 3)(0.02)= 0.293 MPa

    sA = -2538.75

    0.0112 + 0 = -0.2267 MPa = 0.227 MPa (C)

    A. y = 0.

    s =N

    A +My

    I

    QA = y1A1 + y1A2 = 0.065(0.13)(0.2) + 0.14(0.02)(0.15) = 0.589(10- 3) m3

    I =1

    12(0.15)(0.33) -

    1

    12(0.13)(0.263) = 0.14709(10- 3) m4

    A = 0.15(0.3) - 0.13(0.26) = 0.0112 m2

    M = 3947.00 N # m

    2931.50 sin 30(2) + 2931.50 cos 30(0.4) - M = 0+ MO = 0;

    V = 1465.75 N2931.50 sin 30 - V = 0+c Fy = 0;

    N = 2538.75 NN - 2931.50 cos 30 = 0:+ Fx = 0;

    FDE = 2931.50 N

    FDE sin 30(6) + FDE cos 30(0.4) - 500(9.81)(2) = 0+MC = 0;

    *840. The 500-kg engine is suspended from the jib crane atthe position shown. Determine the state of stress at pointAon the cross section of the boom at section aa.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    Section a a

    20 mm

    20 mm

    20 mm

    150 mm

    150 mm

    300 mmA

    B

    E

    C

    D

    2 m2 m 2 m

    0.4 m

    30a

    a

    a

    a

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    776

    840. Continued

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

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    777

    Support Reactions: Referring to the free-body diagram of the entire boom, Fig.a,

    Internal Loadings: Considering the equilibrium of the free-body diagram of thebooms right cut segment, Fig.b,

    Section Properties: The cross-sectional area and the moment of inertia about thecentroidal axis of the booms cross section are

    Referring to Fig. c, QBis

    Normal Stress: The normal stress is the combination of axial and bending stress.Thus,

    For point Then

    Ans.sB = -2538.75

    0.0112 +

    3947.00(0.13)

    0.14709(10 - 3)= 3.26 MPa (T)

    B, y = 0.13 m.

    s =N

    A +My

    I

    QB = y2A2 = 0.14(0.02)(0.15) = 0.42(10

    - 3) m3

    I =1

    12(0.15)(0.33) -

    1

    12(0.13)(0.263) = 0.14709(10- 3) m4

    A = 0.15(0.3) - 0.13(0.26) = 0.0112 m2

    M = 3947.00 N # m

    2931.50 sin 30(2) + 2931.50 cos 30(0.4) - M = 0+ MO = 0;

    V = 1465.75 N2931.50 sin 30 - V = 0+ c Fy = 0;

    N = 2538.75 NN - 2931.50 cos 30 = 0:+ Fx = 0;

    FDE = 2931.50 N

    FDE sin 30(6) + FDE cos 30(0.4) - 500(9.81)(2) = 0+MC = 0;

    841. The 500-kg engine is suspended from the jib crane atthe position shown. Determine the state of stress at pointBon the cross section of the boom at section aa. Point B is

    just above the bottom flange.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    Section a a

    20 mm

    20 mm

    20 mm

    150 mm

    150 mm

    300 mmA

    B

    E

    C

    D

    2 m2 m 2 m

    0.4 m

    30a

    a

    a

    a

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    778

    841. Continued

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    Shear Stress: The shear stress is contributed by transverse shear stress only.Thus,

    Ans.

    The state of stress at point Bis represented on the element shown in Fig. d.

    tB = VQB

    It =

    1465.75[0.42(10- 3)]

    0.14709(10 - 3)(0.02)= 0.209 MPa

    Ans:

    sB = 3.26 MPa (T), tB = 0.209 MPa

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    779

    Internal Loadings: Considering the equilibrium of the free-body diagramof the posts upper cut segment, Fig.a,

    Section Properties: The moments of inertia about theyandzaxes and thepolar moment of inertia of the posts cross section are

    Referring to Fig. b,

    Normal Stress: The normal stress is contributed by bending stress only.Thus,

    For point and Then

    Ans.sA = -0 + -2000(12)(-2.5)

    5.765625p= 3.31 ksi (T)

    z = -2.5 in.A, y = 0

    s = -Mzy

    Iz+

    Myz

    Iy

    (Qy)A =4(2.5)

    3p cp

    2(2.52) d - 4(2)

    3p cp

    2(22) d = 5.0833 in3

    (Qz)A = 0

    J = p

    2(2.54 - 24) = 11.53125pin4

    Iy = Iz = p

    4

    (2.54 - 24) = 5.765625pin4

    Mz = 1500 lb # ftMz = 0; Mz - 300(5) = 0My = -2000 lb # ftMy = 0; My + 400(5) = 0T = -600 lb # ftMx = 0; T + 400(1.5) = 0Vz = -400 lbFz = 0; Vz + 400 = 0

    Vy = -300 lbFy = 0; Vy + 300 = 0

    842. Determine the state of stress at point A on the crosssection of the post at section aa. Indicate the results on adifferential element at the point.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    a a

    5 ft

    1.5 ft

    300 lb400 lb

    2 in.

    2.5 in.

    A

    B

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    780

    842. Continued

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    Shear Stress: The torsional shear stress at pointsA and Bare

    The transverse shear stresses at pointsA and Bare

    Combining these two shear stress components,

    Ans.

    Ans.

    The state of stress at pointA is represented on the element shown in Fig. c.

    (txz)A = 0

    (t

    xy)A = [(t

    xy)T]A + [(t

    xy)V]A = 0.4969 + 0.08419 = 0.581 ksi

    [(txy)V]A =Vy(Qy)B

    Iz t =

    300(5.0833)

    5.765625p(5 - 4) = 0.08419 ksi

    [(txz)V]A =Vz(Qz)A

    Iy t = 0

    [(txy)T]A = Tc

    J =

    600(12)(2.5)

    11.53125p= 0.4969 ksi

    Ans:

    sA = 3.31 ksi (T), tA = 0.581 ksi

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    781

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    a a

    5 ft

    1.5 ft

    300 lb400 lb

    2 in.

    2.5 in.

    A

    B

    Internal Loadings: Considering the equilibrium of the free-body diagram of theposts upper segment, Fig.a,

    Section Properties: The moments of inertia about theyand zaxes and the polarmoment of inertia of the posts cross section are

    Referring to Fig. b,

    Normal Stress: The normal stress is contributed by bending stress only.Thus,

    For point in. and . Then

    Ans.sB =1500(12)(2)

    5.765625p+ 0 = -1.987 ksi = 1.99 ksi (C)

    z = 0B, y = 2

    s = -Mzy

    Iz+Myz

    Iy

    (Qz)B =4(2.5)

    3p cp

    2(2.52) d - 4(2)

    3p cp

    2(22) d = 5.0833 in3

    (Qy)B = 0

    J = p

    2(2.54 - 24) = 11.53125pin4

    Iy = Iz = p

    4(2.54 - 24) = 5.765625pin4

    Mz = 1500 lb # ftMz = 0; Mz - 300(5) = 0My = -2000 lb # ftMy = 0; My + 400(5) = 0T = -600 lb # ftMx = 0; T + 400(1.5) = 0Vz = -400 lb

    Fz = 0; Vz + 400 = 0

    Vy = -300 lbFy = 0; Vy + 300 = 0

    843. Determine the state of stress at point B on the crosssection of the post at section aa. Indicate the results on adifferential element at the point.

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    782

    843. Continued

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    Shear Stress: The torsional shear stress at point Bis

    The transverse shear stress at point Bis

    Combining these two shear stress components,

    Ans.

    Ans.

    The state of stress at point Bis represented on the element shown in Fig. c.

    (txy)B = 0

    (txz)B = [(txz)T]B + [(txz)V]B = 0.3975 + 0.1123 = 0.510 ksi

    [(txz)V]B =Vz(Qz)B

    Iy t =

    400(5.0833)

    5.765625p(5 - 4) = 0.1123 ksi

    [(txy)V]B =Vy(Qy)A

    Iz t = 0

    [(txz)T]B = Tc

    J =

    600(12)(2)

    11.53125p= 0.3975 ksi

    Ans:

    sB = 1.99 ksi (C), tB = 0.510 ksi

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    783

    Referring to Fig. a,

    The cross-sectional area and moments of inertia about they and z axes of the crosssection are

    The normal stress developed is the combination of axial and bending stress.Thus,

    For pointA, . and .

    Ans.

    For point B, and .

    Ans.= -3.00 ksi = 3.00 ksi (C)

    sB = -18.018.0

    - 18.0(3)54

    + -9.00(1.5)13.5

    z = 1.5 iny = 3 in

    = -1.00 ksi = 1.00 ksi (C)

    sA = -18.0

    18.0 -

    18.0(3)

    54.0 +

    -9.00(-1.5)

    13.5

    z = -1.5 iny = 3 in

    s = F

    A -

    Mzy

    Iz+Myz

    Iy

    Iz =1

    12(3)(63) = 54.0 in4

    Iy =1

    12(6)(3)3 = 13.5 in4

    A = 6(3) = 18 in2

    Mz = (MR)z;

    12(3) - 6(3) = Mz

    Mz = 18.0 kip # in

    My = (MR)y;6(1.5) - 12(1.5) = MyMy = -9.00 kip # in

    Fx = (FR)x;-6 - 12 = F F = -18.0 kip

    *844. Determine the normal stress developed at pointsAand B. Neglect the weight of the block.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    a

    a

    6 in.

    6 kip

    12 kip3 in.

    A B

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    784

    Referring to Fig. a,

    The cross-sectional area and the moment of inertia about the y and z axes of thecross section are

    The normal stress developed is the combination of axial and bending stress.Thus,

    For pointA, . and .

    Ans.

    For point B, . and .

    Ans.= -3.00 ksi = 3.00 ksi (C)

    sB = -18.0

    18.0 -

    18.0(3)

    54.0 +

    -9.00(1.5)

    13.5

    z = 1.5 iny = 3 in

    = -1.00 ksi = 1.00 ksi (C)

    sA = -18.0

    18.0 - 18.0(3)

    54.0 + -9.00(-1.5)

    13.5

    z = -1.5 iny = 3 in

    s = F

    A -

    Mzy

    Iz+Myz

    Iy

    Iz =1

    12(3)(63) = 54.0 in4

    Iy =1

    12(6)(33) = 13.5 in4

    A = 3 (6) = 18.0 in2

    Mz = (MR)z; 12(3) - 6(3) = MzMz = 18.0 kip # in

    My = (MR)y; 6(1.5) - 12(1.5) = MyMy = -9.00 kip # in

    Fx = (FR)x; -6 - 12 = FF = -18.0 kip

    845. Sketch the normal stress distribution acting over thecross section at section aa. Neglect the weight of the block.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    a

    a

    6 in.

    6 kip

    12 kip3 in.

    A B

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    785

    For point C, and .

    Ans.

    For point D, . and .

    Ans.

    The normal stress distribution over the cross section is shown in Fig.b

    = 1.00 ksi (T)

    sD = -18.0

    18.0

    -18.0(-3)

    54.0

    + -9.00(-1.5)

    13.5

    z = -1.5 iny = -3 in

    = -1.00 ksi = 1.00 ksi (C)

    sC = -18.0

    18.0 -

    18.0(-3)

    54.0 +

    -9.00(1.5)

    13.5

    z = 1.5 iny = -3 in.

    845. Continued

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    Ans:

    sA = 1.00 ksi (C), sB = 3.00 ksi (C)

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    792

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    Equivalent Force System: As shown on FBD.

    Section Properties:

    Normal Stress:

    At point B where and , we require .

    Ans.

    When

    When

    Repeat the same procedures for point A, C and D. The region where P can beapplied without creating tensile stress at points A,B,C, and D is shown shaded inthe diagram.

    ey = 0,

    ez 65

    18a

    ez = 0,

    ey 6 56

    a

    6ey + 18ez 6 5a

    0 7 -5a+ 6ey + 18ez

    0 7P

    30a4 C -5a2 - 6(-a) ey - 18( -a)ez D

    sB 6 0z = -ay = -a

    =P

    30a4 A -5a2 - 6eyy - 18ezz B

    =-P

    6a2 -

    Peyy

    5a4 -

    Pezz

    53a

    4

    s =N

    A -

    Mzy

    Iz+

    Myz

    Iy

    =5

    3a4

    Iy =1

    12(2a)(2a)3 + 2B 1

    36(2a)a3 +

    1

    2(2a)aa a

    3b2R

    = 5a4

    Iz =1

    12(2a)(2a)3 + 2B 1

    36(2a)a3 +

    1

    2(2a)aaa + a

    3b2R

    A = 2a(2a) + 2B12

    (2a)aR = 6a2

    851. A post having the dimensions shown is subjected tothe bearing load P. Specify the region to which this load canbe applied without causing tensile stress to be developed atpoints A, B, C, and D.

    x

    y

    z

    A

    a a a a

    a

    a

    D

    ez

    eyBC

    P

    Ans:

    6ey + 18ez 6 5a

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    796

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    Internal Loadings: Considering the equilibrium of the free-body diagram of theposts upper segment, Fig.a,

    Section Properties: The moment of inertia about they and z axes of the posts crosssection is

    Referring to Fig.b,

    Normal Stress: The normal stress is contributed by bending stress only.Thus,

    For point and . Then

    Ans.

    Shear Stress: Then transverse shear stress at point A is

    Ans.

    Ans.

    The state of stress at point A is represented on the elements shown in Figs.cand d,respectively.

    [(txz)V]A =Vz(Qz)A

    Iyt =

    4(103)[0.125(10- 3)]

    8.3333(10 - 6)(0.1)= 0.6 MPa

    [(txy)V]A =Vy(Qy)A

    Izt = 0

    sA =1.2(103)(-0.05)

    8.3333(10 - 6)+ 0 = 7.20 MPa (T)

    z = 0A, y = -0.05 m

    s = -Mzy

    Iz+

    Myz

    Iy

    (Qz)A = 0.025(0.05)(0.1) = 0.125(10- 3) m3

    (Qy)A = 0

    Iy = Iz =1

    12(0.1)(0.13) = 8.3333(10 - 6) m4

    Mz = -1.2 kN # mMz = 0; Mz - 3(0.4) = 0

    My = -1.6 kN # mMy = 0; My + 4(0.4) = 0

    Mx = 0; T = 0

    Vz = -4 kNFz = 0; Vz + 4 = 0

    Vy = -3 kNFy = 0; Vy + 3 = 0

    855. Determine the state of stress at pointA on the crosssection of the post at section aa. Indicate the results on adifferential element at the point.

    400 mm

    3 kN4 kN

    100 mm100 mm

    400 mm

    a

    yx

    a

    z

    50 mm

    50 mm

    50 mm

    50 mm BA

    Section a a

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    797

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    855. Continued

    Ans:

    sA = 7.20 MPa (T), tA = 0.6 MPa

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    798

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    Internal Loadings: Considering the equilibrium of the free-body diagram of theposts upper segment, Fig.a,

    Section Properties: The moment of inertia about theyand zaxes of the posts crosssection is

    Referring to Fig.b,

    Normal Stress: The normal stress is contributed by bending stress only.Thus,

    For point and . Then

    Ans.

    Shear Stress: Then transverse shear stress at point Bis

    Ans.

    Ans.

    The state of stress at point Bis represented on the elements shown in Figs.cand d,respectively.

    c(txy)V dB

    =

    Vy(Qy)A

    Izt =

    3(103)[0.125(10- 3)]

    8.3333(10- 6)(0.1)= 0.45 MPa

    c(txy)V dB

    =Vz(Qz)A

    Iyt = 0

    sB = -0 +-1.6(103)(-0.05)

    8.3333(10 - 6)= 9.60 MPa (T)

    z = -0.05 mB, y = 0

    s = -Mzy

    Iz+

    Myz

    Iy

    (Qy)B = 0.025(0.05)(0.1) = 0.125(10- 3) m3

    (Qz)B = 0

    Iy = Iz =1

    12(0.1)(0.13) = 8.3333(10- 6) m4

    Mz = 1.2 kN # mMz = 0; Mz - 3(0.4) = 0

    My = -1.6 kN # mMy = 0; My + 4(0.4) = 0

    Mx = 0; T = 0

    Vz = -4 kNFz = 0; Vz + 4 = 0

    Vy = -3 kNFy = 0; Vy + 3 = 0

    *856. Determine the state of stress at point B on the crosssection of the post at section aa. Indicate the results on adifferential element at the point.

    400 mm

    3 kN4 kN

    100 mm100 mm

    400 mm

    a

    yx

    a

    z

    50 mm

    50 mm

    50 mm

    50 mm BA

    Section a a

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    799

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    856. Continued

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    802

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    859. If determine the maximum normal stressdeveloped on the cross section of the column.

    P = 60 kN,

    100 mm

    15 mm

    15 mm

    15 mm

    75 mm

    150 mm

    150 mm

    100 mm

    100 mm

    P

    2P

    Equivalent Force System: Referring to Fig. a,

    Section Properties: The cross-sectional area and the moment of inertia about the yand zaxes of the cross section are

    Normal Stress: The normal stress is the combination of axial and bending stress.Here, F is negative since it is a compressive force. Also, and are negativesince they are directed towards the negative sense of their respective axes. Byinspection, pointA is subjected to a maximum normal stress.Thus,

    Ans.= -71.0 MPa = 71.0 MPa (C)

    smax = sA = -180(103)

    0.01005 -

    [-30(103)](-0.15)

    0.14655(10 - 3)+

    [-4.5(103)](0.1)

    20.0759(10 - 6)

    s =N

    A -

    Mzy

    Iz+Myz

    Iy

    MzMy

    Iy = 2 c 112

    (0.015)(0.23) d + 112

    (0.27)(0.0153) = 20.0759(10 - 6) m4

    Iz =1

    12(0.2)(0.33) -

    1

    12(0.185)(0.273) = 0.14655(10 - 3) m4

    A = 0.2(0.3) - 0.185(0.27) = 0.01005 m2

    Mz = (MR)z; -120(0.25) = -Mz Mz = 30 kN # m

    My = (MR)y; -60(0.075) = -My My = 4.5 kN # m

    + c Fx = (FR)x; -60 - 120 = -F F = 180 kN

    Ans:

    smax = 71.0 MPa (C)

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    803

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    Equivalent Force System: Referring to Fig. a,

    Section Properties: The cross-sectional area and the moment of inertia about the yand zaxes of the cross section are

    Normal Stress: The normal stress is the combination of axial and bending stress.Here, F is negative since it is a compressive force. Also, and are negativesince they are directed towards the negative sense of their respective axes. Byinspection, point A is subjected to a maximum normal stress, which is incompression. Thus,

    Ans.P = 84470.40 N = 84.5k N

    -100(106) = - 3P

    0.01005 -

    (-0.5P)(-0.15)

    0.14655(10 - 3)+

    -0.075P(0.1)

    20.0759(10 - 6)

    s =N

    A -

    Mzy

    Iz+Myz

    Iy

    MzMy

    Iy = 2 c1

    12(0.15)(0.23) d +1

    12(0.27)(0.0153) = 20.0759(10 - 6) m4

    Iz =1

    12(0.2)(0.33) -

    1

    12(0.185)(0.273) = 0.14655(10- 3)m4

    A = 0.2(0.3) - 0.185(0.27) = 0.01005m2

    Mz = 0.5P

    Mz = (MR)z; -2P(0.25) = -Mz

    My = 0.075P

    My = (MR)y; -P(0.075) = -My

    F = 3P

    + c Fx = (FR)x; -P - 2P = -F

    *860. Determine the maximum allowable force P, if thecolumn is made from material having an allowable normalstress of .sallow = 100 MPa

    100 mm

    15 mm

    15 mm

    15 mm

    75 mm

    150 mm

    150 mm

    100 mm

    100 mm

    P

    2P

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    822

    Support Reactions: Referring to the free-body diagram of member BC shown inFig. a,

    a

    Internal Loadings: Consider the equilibrium of the free-body diagram of the right

    segment shown in Fig. b.

    By = 196.2N554.94 sin45 - 20(9.81) - By = 0+ c Fy = 0;

    Bx = 392.4N554.94 cos45 - Bx = 0:+ Fx = 0;

    F = 554.94NFsin45(1) - 20(9.81)(2) = 0+ MB = 0;

    875. The 20-kg drum is suspended from the hook mountedon the wooden frame. Determine the state of stress at pointEon the cross section of the frame at section aa. Indicate theresults on an element.

    2014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved.This material is protected under all copyright laws as they currentlyexist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

    a M = 98.1N # m196.2(0.5) - M = 0+ MC = 0;

    V = 196.2NV - 196.2 = 0+ c Fy = 0;

    N = 392.4NN - 392.4 = 0:+ Fx = 0;

    Section Properties: The cross -sectional area and the moment of inertia of the crosssection are

    Referring to Fig. c,QE is

    Normal Stress: The normal stress is the combination of axial and bending stress.Thus,

    For point E, . Then

    Ans.

    Shear Stress: The shear stress is contributed by transverse shear stress only.Thus,

    Ans.

    The state of stress at point E is represented on the element shown in Fig.d.

    tE = VQA

    It =

    196.2 C31.25 A10- 6 B D

    1.7578 A10- 6 B(0.05)= 69.8 kPa

    sE =

    392.4

    3.75 A10- 3 B +98.1(0.0125)

    1.7578 A10 - 6 B = 802 kPa

    y = 0.0375 - 0.025 = 0.0125m

    s =N

    A ;My

    I

    QE = yA = 0.025(0.025)(0.05) = 31.25 A10- 6 B m3

    I =1

    12(0.05) A0.0753 B = 1.7578 A10- 6 B m4

    A = 0.05(0.075) = 3.75 A10- 3 B m2

    1 m

    1 m

    1 m

    b

    a

    a

    b

    CB

    A

    30

    1 m0.5 m0.5 m

    50 mm

    75 mm

    25 mm

    Section a a

    E

    75 mm

    75 mm

    25 mm

    Section b b

    FD

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    823

    875. Continued

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    Ans:

    sE = 802 kPa, tE = 69.8 kPa

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    824

    Support Reactions: Referring to the free-body diagram of the entire frame shown inFig. a,

    a

    Internal Loadings: Consider the equilibrium of the free-body diagram of the lowercut segment,Fig.b,

    a

    Section Properties: The cross -sectional area and the moment of inertia about thecentroidal axis of the cross section are

    Referring to Fig. c,QE is

    Normal Stress: The normal stress is the combination of axial and bending stress.Thus,

    For point F, . Then

    Ans.= -695.24 kPa = 695 kPa (C)

    sF = -422.75

    5.625 A10 - 3 B -

    130.8(0.0125)

    2.6367 A10 - 6 B

    y = 0.0375 - 0.025 = 0.0125 m

    s =N

    A ;My

    I

    QF = yA = 0.025(0.025)(0.075) = 46.875 A10- 6

    B m3

    I =1

    12(0.075) A0.0753 B = 2.6367 A10- 6 B m4

    A = 0.075(0.075) = 5.625 A10- 3 B m2

    M = 130.8N # m130.8(1) - M = 0+ MC = 0;

    N = 422.75N422.75 - N = 0+ c Fy = 0;

    V = 130.8N130.8 - V = 0:+ Fx = 0;

    Ax = 130.8NAx - 261.6sin30 = 0:+ Fx = 0;

    Ay = 422.75NAy - 261.6cos30 - 20(9.81) = 0+ c Fy = 0;

    FBD = 261.6NFBDsin30(3) - 20(9.81)(2) = 0+ MA = 0;

    *876. The 20-kg drum is suspended from the hookmounted on the wooden frame. Determine the state of stressat point Fon the cross section of the frame at section .Indicate the results on an element.

    b-b

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    1 m

    1 m

    1 m

    b

    a

    a

    b

    CB

    A

    30

    1 m0.5 m0.5 m

    50 mm

    75 mm

    25 mm

    Section a a

    E

    75 mm

    75 mm

    25 mm

    Section b b

    FD

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    825

    Shear Stress: The shear stress is contributed by transverse shear stress only.Thus,

    Ans.

    The state of stress at point A is represented on the element shown in Fig.d.

    tA = VQA

    It =

    130.8 c46.875 A10- 6

    Bd2.6367 A10- 6 B(0.075)

    = 31.0 kPa

    876. Continued

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    834

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    a

    At point C,

    Ans.

    Ans.

    At point D,

    Ans.

    Ans.tD = 0

    sD = P

    A

    - Mc

    I

    =2(5.80)

    1

    -[2(5.80)](1)

    0.333

    = -23.2 ksi

    tC = 0

    sC = P

    A =

    2(5.80)

    1 = 11.6 ksi

    A = 2(0.25)(2) = 1 in2

    I = 2 c 112

    (0.25)(2)3 d = 0.333 in4FA = 11.60 kip

    + MB = 0 ; 12(3) + 10(8) - FA(10) = 0

    885. The wall hanger has a thickness of 0.25 in. and isused to support the vertical reactions of the beam that isloaded as shown. If the load is transferred uniformly to eachstrap of the hanger, determine the state of stress at pointsCand D on the strap at A. Assume the vertical reactionF atthis end acts in the center and on the edge of the bracketas shown.

    10 kip

    A B

    2 kip/ft

    2 ft 2 ft 6 ft

    2 in.

    3.75 in.

    2.75 in.

    3 in.

    1 in.

    2 in.

    2 in.

    F

    CD

    1 in.

    Ans:

    sD = -23.2 ksi, tD = 0

    sC = 11.6 ksi, tC = 0,

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    a

    At point C:

    Ans.

    Ans.

    At point D:

    Ans.

    Ans.tD = 0

    sD = P

    A -Mc

    I =

    2(5.20)

    1 -

    [2(5.20)](1)

    0.333 = -20.8 ksi

    tC = 0

    sC = P

    A =

    2(5.20)

    1 = 10.4 ksi

    I = 2 c 112

    (0.25)(2)3 d = 0.333 in4; A = 2(0.25)(2) = 1 in2+ MA = 0; FB(10) - 10(2) - 12(7) = 0; FB = 10.40 kip

    886. The wall hanger has a thickness of 0.25 in. and isused to support the vertical reactions of the beam that isloaded as shown. If the load is transferred uniformly to eachstrap of the hanger,determine the state of stress at pointsCand D on the strap at B. Assume the vertical reaction F atthis end acts in the center and on the edge of the bracketas shown.

    10 kip

    A B

    2 kip/ft

    2 ft 2 ft 6 ft

    2 in.

    3.75 in.

    2.75 in.

    3 in.

    1 in.

    2 in.

    2 in.

    F

    CD

    1 in.

    Ans: