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    Chapter-2: Slope Deflection Method

    By Prof. H.P.Sudarshan

    Sri Siddhartha Institute Of Tech,Tumkur 

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    Example:  Analyze the propped cantilever shown by using slope defection

    method. Then draw Bending moment and shear force diagram.

    Solution: End A is fixed hence  A =0

    End B is Hinged hence B ≠0

     Assume both ends are fixed and therefore fixed end moments are

    12wLF,

    12wLF

    2

    BA

    2

     AB  

    The Slope deflection equations for final moment at each end are

    )2(L

    EI4

    12

    wL

    2L

    EI2FM

    )1(L

    EI2

    12

    wL

    2L

    EI2FM

    B

    2

     ABBABA

    B

    2

    B A AB AB

    In the above equations there is only one unknown B .

    To solve we have boundary condition at B;

    Since B is simply supported, the BM at B is zero

    ie. MBA=0.

    iseanticlockwisrotationtheindicatessignve-48

    wLEI

    0L

    EI4

    12

    wLM(2)equationFrom

    3

    B

    B

    2

    BA

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    Substituting the value of  BEI in equation (1) and (2) we have end moments

    048

    wL

    L

    4

    12

    wL

    M

    anticlockwismomentindicatessignve-8

    wL

    48

    wL

    L

    2

    12

    wLM

    32

    BA

    232

     AB

     

     

     

     

     

      

     

    MBA has to be zero, because it is hinged.

    Now consider the free body diagram of the beam and find reactions using

    equations of equilibrium.

    wL8

    3

    wL85wLRwLR

    wLRR

    0V

    wL8

    5R

    wL8

    5

    2

    LwL

    8

    wL

    2

    LwLMLR

    0M

     AB

    B A

     A

    2

     AB A

    B

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    Problem can be treated as

    The bending moment diagram for the given problem is as below

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    The max BM occurs where SF=0. Consider SF equation at a distance of x

    from right support

    2

    2

    Xmax

    X

    wL128

    9

    L8

    3

    2

    wL

    8

    3wL

    8

    3MM

    BsupportfromL8

    3atoccursBMmaxtheHence

    L83X

    0wXwL8

    3S

     

      

     

     And point of contra flexure occurs where BM=0, Consider BM equation ata distance of x from right support.

    L4

    3X

    02

    XwwLX

    8

    3M

    2

    X

    For shear force diagram, consider SF equation from B

    wL8

    5SLS

    wL8

    3S0S

    wXwL

    8

    3S

     AX

    BX

    X

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    Example:  Analyze two span continuous beam ABC by slope deflection method.

    Then draw Bending moment & Shear force diagram. Take EI constant

    Solution: Fixed end moments are:

    KNM67.4112

    520

    12

    wLF

    KNM67.4112

    520

    12

    wLF

    KNM89.886

    24100

    L

    bWaF

    KNM44.446

    24100

    L

    WabF

    22

    CB

    22

    BC

    2

    2

    2

    2

    BA

    2

    2

    2

    2

     AB

    Since A is fixed 0 A   , ,0,0 CB  

    Slope deflection equations are:

    )2(EI3

    289.88

    62EI289.88

    2L

    EI2FM

    )1(EI3

    144.44

    6

    EI244.44

    2L

    EI2FM

    B

    B

     ABBABA

    B

    B

    B A AB AB

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    )4(EI5

    2

    5

    EI467.41

    25

    EI267.41

    2L

    EI2FM

    )3(EI5

    2EI5

    467.41

    25

    EI267.41

    2L

    EI2FM

    BC

    BC

    BCCBCB

    CB

    CB

    CBBCBC

    In all the above four equations there are only two unknown B and C . And

    accordingly the boundary conditions are

    i -MBA-MBC=0

    MBA+MBC=0

    ii MCB=0 since C is end simply support.

    )6(0EI5

    4EI

    5

    267.41M

    )5(0EI5

    2EI

    15

    2222.47

    EI52EI

    5467.41EI

    3289.88MMNow

    CBCB

    CB

    CBBBCBA

    Solving simultaneous equations 5 & 6 we get

    EI B = – 20.83 Rotation anticlockwise.

    EI C = – 41.67 Rotation anticlockwise.

    Substituting in the slope definition equations

    M AB = – 44.44 +   KNM38.5183.203

    1

    MBA = + 88.89 +   KNM00.7583.203

    2

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    MBC = – 41.67+   KNM00.7567.415

    283.20

    5

    4

    MCB = + 41.67+   067.415

    483.20

    5

    2

    Reactions: Consider the free body diagram of the beam.

    Find reactions using equations of equilibrium.

    Span AB: ΣM A = 0 RB×6 = 100×4+75-51.38

    RB = 70.60 KN

    ΣV = 0 R A+RB = 100KN

    R A = 100-70.60=29.40 KN

    Span BC: ΣMC = 0 RB×5 = 20×5×2

    5+75

    RB = 65 KN

    ΣV=0 RB+RC = 20×5 = 100KN

    RC = 100-65 = 35 KN

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    Using these data BM and SF diagram can be drawn.

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    Max BM:

    Span AB: Max BM in span AB occurs under point load and can be found

    geometrically

    Mmax=113.33-51.38 -

    KNM20.4646

    38.5175

    Span BC:Max BM in span BC occurs where shear force is zero or 

    changes its sign. Hence consider SF equation w.r.t C

    Sx = 35-20x= 020

    35x  =1.75m

    Max BM occurs at 1.75m from C

    Mmax = 35 × 1.75 – 20

    2

    75.1 2 = 30.625 KNM

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    Example: Analyze continuous beam ABCD by slope deflection method and thendraw bending moment diagram. Take EI constant.

    Solution:

    0,0,0 CB A  

    FEMS MKN44.44-6

    24100L

    WabF 2

    2

    2

    2

     AB  

    KNM88.886

    24100

    L

    bWaF

    2

    2

    2

    2

    BA  

    KNM41.67-12

    520

    12

    wLF

    22

    BC 

    KNM41.6712

    520

    12

    wLF

    22

    CB 

    MKN30-5.120FCD  

    Slope deflection equations:

    1---------EI3

    144.442

    L

    EI2FM BB A AB AB  

    2---------EI3

    289.882

    L

    EI2FM B ABBABA  

    3--------EI5

    2EI

    5

    467.412

    L

    EI2FM CBCBBCBC  

    4--------EI5

    2EI

    5

    467.412

    L

    EI2FM BCBCCBCB  

    KNM30MCD  

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    In the above equations we have two unknown rotations CB and   , accordingly

    the boundary conditions are:

    0MM

    0MM

    CDCB

    BCBA

    5--------0EI5

    2EI

    15

    2222.47

    EI5

    2EI

    5

    467.41EI

    3

    289.88MM,Now

    CB

    CBBBCBA

    6EI54EI5267.11

    30EI5

    2EI

    5

    467.41MM, And

    CB

    BCCDCB

    Solving (5) and (6) we get

    [email protected]

    [email protected]

    C

    B

    Substituting value of  BEI and CEI in slope deflection equations we have

    KNM30M

    KNM00.3067.325

    275.1

    5

    467.41M

    KNM11.6775.15

    267.32

    5

    467.41M

    KNM11.6767.323

    289.88M

    KNM00.6167.322144.44M

    CD

    CB

    BC

    BA

     AB

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    Reactions: Consider free body diagram of beam AB, BC and CD as shown

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     ABSpan

    KN31.32R100R

    KN69.67R

    6111.6741006R

    B A

    B

    B

    BCSpan

    KN42.57R520R

    KN58.42R

    11.673052

    5205R

    BB

    C

    C

    Maximum Bending Moments:

    Span AB: Occurs under point load

     

      

     

    KNM26.684

    6

    6111.676133.133Max

    Span BC: where SF=0, consider SF equation with C as reference

    m13.220

    58.42x

    0x2058.42SX

    MKN26.15302

    13.22013.258.42M

    2

    max  

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    Example:  Analyse the continuous beam ABCD shown in figure by slope

    deflection method. The support B sinks by 15mm.

    Take 4625 m10120Iandm/KN10200E  

    Solution:

    In this problem  A =0,   B 0,   C 0,   =15mm

    FEMs:

    KNM44.44L

    WabF

    2

    2

     AB 

    KNM89.88L

    bWaF

    2

    2

    BA 

    KNM67.418

    wLF

    2

    BC  

    KNM67.418

    wLF

    2

    CB  

    FEM due to yield of support B

    For span AB:

    KNM61000

    151012010

    6

    2006

    LEI6mm

    65

    2

    2baab

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    For span BC:

    KNM64.81000

    151012010

    5

    2006

    L

    EI6mm

    65

    2

    2cbbc

    Slope deflection equation

    5---------KNM30M

    4---------EI5

    2EI

    5

    431.50

    64.82EI5

    241.67

    L

    EI6)2(

    L

    EI2FM

    3---------EI5

    2EI

    5

    403.33

    64.82EI5

    2

    41.67-

    L

    EI6)2(

    L

    EI2FM

    2---------EI3

    289.82

    6EI3

    288.89

    L

    EI6)2(

    L

    EI2FM

    1---------EI

    3

    144.50

    6EI3

    144.44-

    L

    EI62

    L

    EIF

    )L

    32(

    L

    EI2FM

    CD

    BC

    BC

    2BCCBCB

    CB

    CB

    2CBBCBC

    B

    B

    2 ABBABA

    B

    B

    2B A AB

    B A AB AB

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    There are only two unknown rotations B and C . Accordingly the boundaryconditions are

    Now,

    0EI5

    4EI

    5

    231.20MM

    0EI52EI

    152286.49MM

    0MM

    0MM

    CBCDCB

    CBBCBA

    CDCB

    BCBA

    Solving these equations we get

    ockwise  Anticl71.9EI

    ockwise  Anticl35.31EI

    C

    B

    Substituting these values in slope deflections we get the final moments:

    KNM30M

    KNM00.3035.315

    271.9

    5

    431.50M

    KNM99.6171.95

    235.31

    5

    403.33M

    KNM99.6135.313

    289.82M

    KNM89.6035.313

    144.50M

    CD

    CB

    BC

    BA

     AB

    Consider the free body diagram of continuous beam for finding reactions

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    Reactions:

    Span AB:RB × 6 = 100 x 4 + 61.99 – 60.89

    RB = 66.85

    R A = 100 – RB

    =33.15 KN

    Span BC:

    RB × 5 = 20 x 5 x2

    5+ 61.99 – 30

    RB = 56.40 KN

    RC = 20 x 5 - RB

    =43.60 KN

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    Example: Three span continuous beam ABCD is fixed at A and continuous over 

    B, C and D. The beam subjected to loads as shown. Analyse the beam by slope

    deflection method and draw bending moment and shear force diagram.

    Solution:

    Since end A is fixed 0,0,0,0 DcB A  

    FEMs:

    KNM30-8

    460

    8

    WlF AB  

    KNM308

    460

    8

    WlFBA  

    KNM12.54

    MFBC  

    KNM12.54

    MFCB  

    KNM313.3-12

    410

    12

    wl

    F

    22

    CD  

    KNM13.3312

    410

    12

    wlF

    22

    DC  

    Slope deflection equations:

    B A AB AB 2L

    EI2FM  

    04

    EI230- B

    1--------EI0.530- B  

     ABBABA 2L

    EI2FM  

    024

    EI230 B

    2---------EI30 B  

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    CBBCBC 2L

    EI2FM  

    24

    EI212.5 CB  

    3---------EI5.0EI12.5 CB  

    BCCBCB 2L

    EI2FM  

    24

    EI25.12 BC  

    4---------EI5.0EI12.5 BC  

    DCCDCD 2L

    EI2FM  

    24

    EI213.33- DC  

    5----------EI5.0EI33.13 DC  

    CDDCDC 2L

    EI2FM  

    24

    EI213.33 CD  

    6----------EIEI5.013.33 DC  

    In the above Equations there are three unknowns, EI DCB EI&EI,   ,

    accordingly the boundary conditions are:

    )hinged(0Miii

    0MMii

    0MMi

    DC

    CDCB

    BCBA

    Now

    705.42EI5.0EI2

    0EI5.0EI5.12EI30

    0MM

    CB

    CBB

    BCBA

    8083.0EI5.0EI2EI5.00EI5.0EI33.13EI5.0EI5.12

    0MM

    DCB

    DCBC

    BCCB

    0MDC

    90EIEI5.033.13 DC  

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    By solving (7), (8) & (9), we get

    90.18EI

    15.11EI

    04.24EI

    D

    C

    B

    By substituting the values of  DcB and,   in respective equations we get

    KNM090.1815.115.033.13M

    KNM63.1190.185.015.1133.13M

    KNM63.1104.245.015.115.12M

    KNM5.96-11.15.5024.04-12.5M

    KNM96.504.2430M

    KNM02.4204.245.030M

    DC

    CD

    CB

    BC

    BA

     AB

    Reactions: Consider the free body diagram of beam.

    Beam AB:

    KN015.30R60R

    KN985.204

    02.4296.5260R

    B A

    B

    Beam BC:

    downwardisRKN92.13RR

    KN92.134

    96.55063.11R

    BCB

    C

    Beam CD:

    KN91.22R410R

    KN09.174

    63.112410R

    DC

    D

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    Example:  Analyse the continuous beam shown using slope deflection method.

    Then draw bending moment and shear force diagram.

    Solution: In this problem fixedis Aend,0 A  

    FEMs:

    MKN53.33-12

    810

    12

    wlF

    22

     AB  

    KNM53.3312wlF

    2

    BA  

    KNM22.50-8

    630

    8

    WlFBC  

    KNM22.508

    WLFCD  

    Slope deflection equations:

    B A AB AB 2L

    EI2FM  

    08

    I3E253.33- B

    1--------EI4

    353.33- B  

     ABBABA 2L

    EI2FM  

    028

    I3E253.33 B

    2--------EI2353.33 B  

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    CBBCBC 2L

    EI2FM  

    26

    I2E222.5- CB  

    3--------EI32

    EI3

    4

    22.5- CB  

    BCCBCB 2L

    EI2FM  

    26

    I2E222.5 BC  

    4--------EI3

    2EI

    3

    422.5 BC  

    In the above equation there are two unknown CB and   , accordingly the

    boundary conditions are:

    0Mii

    024MMi

    CB

    BCBA

    50EI3

    2EI

    6

    1783.54

    24EI3

    2EI

    3

    45.22EI

    2

    333.5324MM,Now

    CB

    CBBBCBA

    0EI32EI

    345.22Mand BCCB  

    (6)-----------EI3

    125.11EI

    3

    2BC  

    Substituting in eqn. (5)

    clockwiseantirotation432.1715

    658.44EI

    0EI6

    1544.58

    0EI3

    125.11EI

    6

    1783.54

    B

    B

    BB

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    from equation (6)

    iseanticlockwrotation159.8

    432.173

    125.11

    2

    3EI C

    Substituting 159.8EIand432.17EI CB   in the slope deflection equationwe get Final Moments:

    KNM18.27432.172

    333.53M

    KNM-66.4017.432-4

    333.53M

    BA

     AB

    00.0)432.17(32159.8

    345.22M

    KNM18.51159.83

    2432.17

    3

    45.22M

    CB

    BC

    Reactions: Consider free body diagram of beams as shown

    Span AB:

    KN87.44R810R

    KN13.358

    481040.6618.27R

    B A

    B

    Span BC:

    KN47.6R30R

    KN53.236

    33018.51R

    BC

    B

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    Max BM

    Span AB: Max BM occurs where SF=0, consider SF equation with A as origin

    KNM67.36642

    487.410487.487.44M

    m487.4x

    010x-87.44S

    2

    max

    x

    Span BC: Max BM occurs under point load

    MKN41.192

    18.5145MBC max  

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    Example:  Analyse the beam shown in figure. End support C is subjected to an

    anticlockwise moment of 12 KNM.

    Solution: In this problem fixedisend,0 A  

    FEMs:

    KNM67.2612

    420

    12

    wlF

    22

    BC  

    KNM26.6712

    wl

    F

    2

    CB  

    Slope deflection equations:

    B A AB AB 2L

    EI2FM  

    04

    I2E20 B

    1---------EI B  

     ABBABA 2L

    EI2FM  

    024

    I2E20 B

    2---------EI2 B  

    CBBCBC 2L

    EI2FM  

    24

    I5.1E226.67- CB  

    3---------EI4

    3EI

    2

    326.67- CB  

    BCCBCB 2LEI2

    FM  

    24

    I5.1E226.67 BC  

    4---------EI4

    3EI

    2

    326.67 BC  

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    In the above equation there are two unknowns CB and   , accordingly the

    boundary conditions are

    012M

    0MM

    CB

    BCBA

    (5)---------067.26EI4

    3EI

    2

    7

    EI4

    3EI

    2

    367.26EI2MM,Now

    CB

    CBBBCBA

    (6)---------0EI2

    3EI

    4

    367.38

    12EI4

    3EI

    2

    367.2612M,and

    CB

    BCCB

    From (5) and (6)

    72.1425

    846EI

    046EI8

    25

    033.19EI4

    3EI

    8

    3

    067.26EI43EI

    27

    B

    B

    CB

    CB

    From (6)

    iseanticlockwrotationindicatessignve-14.33

    72.144

    367.38

    3

    2EI C

     

      

     

    equationsdeflectionslopeisEIandEIngSubstituti CB  

    KNM12)72.14(4

    3)14.33(

    2

    367.26M

    KNM44.2914.334

    3)72.14(

    2

    367.26M

    KNM42.29)72.14(2EI2M

    KNM72.14EIM

    CB

    BC

    BBA

    B AB

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    Reaction: Consider free body diagrams of beam

    Span AB:

    KN04.11RR

    KN04.114

    44.2972.14R

    B A

    B

    Span BC:

    KN64.29R420R

    KN36.504

    24201244.29R

    BC

    B

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    Example: Analyse the simple frame shown in figure. End A is fixed and ends B &C are hinged. Draw the bending moment diagram.

    Solution:

    In this problem ,0,0,0,0 DCB A  

    FEMS:-

    KNM108

    WLF

    KNM108

    420

    8

    WLF

    KNM67.2612

    420

    12

    wlF

    KNM67.2612

    420

    12

    wlF

    KNM33.53

    6

    42120

    L

    bWaF

    KNM67.1066

    42120

    L

    WabF

    DB

    CD

    22

    CB

    22

    BC

    2

    2

    2

    2

    BA

    2

    2

    2

    2

     AB

    Slope deflections are

    )1(EI3

    267.106

    6

    I2E267.106

    2L

    EI2FM

    BB

    B A AB AB

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    )4(EI4

    3EI

    2

    367.262

    2

    I3

    4

    E267.26

    2L

    EI2FM

    )3(EI4

    3EI

    2

    367.262

    2

    I3

    4

    E267.26

    2L

    EI2FM

    )2(EI3

    433.532

    6

    I2E233.53

    2L

    EI2FM

    BCBC

    BCCBCB

    CBCB

    CBCBBC

    BB

    BBBABA

    )6(EI2

    1EI102

    4

    EI210

    2L

    EI2FM

    )5(EI2

    1EI102

    4

    EI210

    2

    L

    EI2FM

    BDBD

    BDDBDB

    DBDB

    DBBDBD

    In the above equations we have three unknown rotations B , C , D accordingly

    we have three boundary conditions.0MMM BDBCBA  

    0MCB  Since C and D are hinged

    0MDB Now

    (9)-----0EIEI2

    110M

    (8)-----0EI23EI

    436.672M

    (7)-----0EI2

    1EI

    4

    3EI

    6

    2336.66

    EI2

    1EI10EI

    4

    3EI

    2

    367.26EI

    3

    433.53MMM

    DBDB

    CBCB

    DCB

    DBCBBBDBCBA

  • 8/20/2019 Slope Def Vtu

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    Solving equations 7, 8, & 9 we get

    414.14EI

    36.13EI

    83.8EI

    D

    C

    B

    Substituting these values in slope equations

    0)83.8(2

    1)414.14(10M

    KNM38.8)414.14(2

    1)83.8(10M

    0)83.8(43)36.13(

    2367.26M

    KNM94.49)36.13(4

    3)3.8(

    2

    367.26M

    KNM56.41)83.8(3

    433.53M

    KNM56.112)83.8(3

    267.106M

    DB

    BD

    CB

    BC

    BA

     AB

  • 8/20/2019 Slope Def Vtu

    34/89

    Reactions: Consider free body diagram of each members

    Span AB:

    KN83.91R120R

    KN17.286

    212056.11256.41R

    B A

    B

    Span BC:

    KN515.27R420R

    KN485.524

    242094.49R

    BC

    B

    Column BD:

    20HHKN78.12H

    KN92.74

    33.8220H

    D AB

    D

  • 8/20/2019 Slope Def Vtu

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  • 8/20/2019 Slope Def Vtu

    36/89

    Example:  Analyse the portal frame shown in figure and also drawn bending

    moment and shear force diagram

    Solution:Symmetrical problem- Sym frame + Sym loading

    0,0,0,0 DCB A  

    FEMS

    KNM106.67-6

    2480

    6

    4280

    L

    cdW

    L

    abW

    F

    2

    2

    2

    2

    2

    2

    2

    2

    2

    1

    BC

    KNM67.106L

    dcW

    L

    bWaF

    2

    22

    2

    2

    CB  

    Slope deflection equations:

    1--------EI2

    10

    4

    EI202

    L

    EI2FM BBB A AB AB  

    2-------EI024

    EI202

    L

    EI2FM BB ABBABA  

  • 8/20/2019 Slope Def Vtu

    37/89

    3------EI3

    2EI

    3

    467.106)2(

    6

    I2E267.106

    2L

    EI2FM

    CBCB

    CBBCBC

    4------EI3

    2EI

    3

    467.106)2(

    6

    I2E267.106

    2L

    EI2FM

    BCBC

    BCCBCB

    5-------EI)02(4

    EI20

    2L

    EI2FM

    CC

    DCCDCD

    6-------EI2

    1)0(

    4

    EI20

    2

    L

    EI2FM

    CC

    CDDCDC

    In the above equation there are two unknown rotations. Accordingly the boundary

    conditions are

    0MM

    0MM

    CDCB

    BCBA

    Now (7)-------0EI32EI

    3767.106MM CBBCBA  

    (8)-------0EI3

    7EI

    3

    267.106MM CBCDCB  

    Multiply by (7) and (8) by 2

    Clockwise6445

    303.960EI

    0EI3

    45960.03-

    subtracts

    0EI3

    14EI

    3

    434.213

    0EI3

    14EI

    3

    4969.746

    B

    B

    CB

    CB

  • 8/20/2019 Slope Def Vtu

    38/89

    Using equation (7)

    ckwise  Anticlo6464

    3

    767.106

    2

    3-

    EI3

    767.106

    2

    3EI BC

    Here we find CB   . It is obvious because the problem is symmetrical.

    aremomentsFinal

    KNM-32642

    1M

    KNM64M

    KNM64643

    2)64(

    3

    467.106M

    KNM64643264

    3467.106M

    KNM64M

    KNM322

    64M

    DC

    CD

    CB

    BC

    BA

     AB

  • 8/20/2019 Slope Def Vtu

    39/89

    Consider free body diagram’s of beam and columns as shown

    By symmetrical we can write

    KNM80RR

    KNM60RR

    CD

    B A

    Now consider free body diagram of column AB

     Apply

    KN24H

    32644H

    0M

     A

     A

    B

    Similarly from free body diagram of column CD

     Apply

    KN24H

    32644H

    0M

    D

     A

    C

  • 8/20/2019 Slope Def Vtu

    40/89

    Check:

    0HH

    0H

    D A  

    Hence okay

    Note: Since symmetrical, only half frame may be analysed. Using first threeequations

    and taking CB  

  • 8/20/2019 Slope Def Vtu

    41/89

    Example: Analyse the portal frame and then draw the bending moment diagram

    Solution:

    This is a symmetrical frame and unsymmetrically loaded, thus it is an

    unsymmetrical problem and there is a sway

     Assume sway to right.

    Here 0,0,0,0 DBD A  

    FEMS:

    KNM75.938

    3580

    L

    bWaF

    KNM25.568

    3580

    L

    WabF

    2

    2

    2

    2

    CB

    2

    2

    2

    2

    BC

    Slope deflection equations

    2--------EI8

    3EI

    4

    302

    4

    2EI0

    L

    32

    L

    EI2FM

    1--------EI8

    3EI

    2

    1

    4

    30

    4

    2EI0

    L

    32

    L

    EI2FM

    BB

     ABBABA

    BB

    B A AB AB

     

      

       

     

      

       

     

      

       

     

      

       

  • 8/20/2019 Slope Def Vtu

    42/89

    6---------EI8

    3EI

    2

    1

    4

    30

    4

    2EI0

    L32

    LEI2FM

    5---------EI8

    3EI

    4

    302

    4

    2EI0

    L

    32

    L

    EI2FM

    4---------EI4

    1EI

    2

    175.932

    8

    2EI75.93

    2L

    EI2FM

    3---------EI

    4

    1EI

    2

    125.562

    8

    2EI25.56

    2L

    EI2FM

    CC

    CDDCDC

    CC

    DCCDCD

    BCBC

    BCCBCB

    CBCB

    CBBCBC

     

      

       

      

        

     

      

       

     

      

       

    In the above equation there are three unknowns   and, CB , accordingly theboundary conditions are,

    0MMMM

    04

    MM

    4

    MM,e.i

    conditionShear ---0PHH

    0MM

    conditionsintJo0MM

    DCCDBA AB

    DCCDBA AB

    HD A

    CDCB

    BCBA

    70EI8

    3EI

    4

    1EI

    2

    325.56

    0EI4

    1EI

    2

    125.56EI

    8

    3EIMM,Now

    CB

    CBBBCBA

    80EI8

    3EI

    2

    3EI

    4

    175.93

    0EI8

    3EIEI

    4

    1EI

    2

    175.93MM, And

    CB

    CBCCDCB

  • 8/20/2019 Slope Def Vtu

    43/89

    90EI23

    EI2

    3EI2

    3

    EI‘8

    3EI

    2

    1

    EI8

    3EIEI

    8

    3EIEI

    8

    3EI

    2

    1MMMM, And

    CB

    C

    CBBDCCDBA AB

    (8)&(7)inSubstitute

    EIEIEI(9)From CB  

    (7)Eqn

    10-------0EI8

    1EI

    8

    925.56

    0EIEI8

    3EI

    4

    1EI

    2

    325.56

    CB

    CBCB

    )8(Eqn

    11----------0EI8

    9EI

    8

    175.93

    0EIEI8

    3EI

    2

    3EI

    4

    175.93

    CB

    CBCB

    Solving equations (10) & (11) we get 25.41EI B

    By Equation (10)

    5.3775.7825.41EIEIEI

    75.7825.418

    925.568

    EI8

    9

    25.568EI

    CB

    BC

    Hence

    5.37EI,75.78EI,25.41EI CB   Substituting these values in slope deflection equations, we have

  • 8/20/2019 Slope Def Vtu

    44/89

    KNM31.255.378

    375.78

    2

    1M

    KNM69.645.378

    375.78M

    KNM69.6475.414

    175.78

    2

    175.93M

    KNM31.5575.784125.41

    2125.56M

    KNM31.555.378

    325.41M

    KNM69.345.378

    325.41

    2

    1M

    DC

    CD

    CB

    BC

    BA

     AB

    Reactions: consider the free body diagram of beam and columns

    Column AB:

    KN5.224

    31.5569.34H A  

    Span BC:

    17.51R80R

    KN83.288

    38069.6431.55R

    BC

    B

    Column CD:

    5.224

    31.2569.64HD  

  • 8/20/2019 Slope Def Vtu

    45/89

    Check:

    ΣH = 0H A + HD = 022.5 – 22.5 = 0Hence okay

  • 8/20/2019 Slope Def Vtu

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    Example: Frame ABCD is subjected to a horizontal force of 20 KN at joint C asshown in figure. Analyse and draw bending moment diagram.

    Solution:

    Frame is Symmetrical and unsymmetrical loaded hence there is a sway.

     Assume sway towards right

    FEMS

    0FFFFFF DCCDCBBCBA AB  

    Slope deflection equations are

    2EI3

    2EI

    3

    4

    3

    32

    3

    EI2

    L

    32

    L

    EI2FM

    1---------EI3

    2EI

    3

    2

    3

    3

    3

    EI2

    L

    32

    L

    EI2FM

    B

    B

     ABBABA

    B

    B

    B A AB AB

     

      

       

     

     

     

       

     

      

       

     

      

       

  • 8/20/2019 Slope Def Vtu

    47/89

    5EI3

    2EI

    3

    43

    32

    3

    2EI

    L

    32

    L

    EI2FM

    4--------EI5.0EI

    24

    EI2

    2L

    EI2FM

    3--------EI5.0EI

    24

    EI2

    2L

    EI2FM

    C

    C

    DCCDCD

    BC

    BC

    BCCBCB

    CB

    CB

    CBBCBC

     

     

      

       

    6---------EI3

    2EI

    3

    2

    3

    3

    3

    EI2

    L

    32

    L

    EI2FM

    C

    c

    CDDCDC

     

     

    The unknown are   &, C,B . areconditionsboundarythey Accordingl

    060MMMM

    0203

    MM

    3

    MM,e.i

    020HH.III

    0MM.II

    0MM.I

    DCCDBA AB

    DCCDBA AB

    D A

    CDCB

    BCBA

    70EI3

    2EI5.0EI

    3

    7

    EI5.0EIEI3

    2EI3

    4MMNow

    CB

    CBBBCBA

  • 8/20/2019 Slope Def Vtu

    48/89

    80EI3

    2EI

    3

    7EI5.0

    EI3

    2EI

    3

    4EI5.0EIMMand

    CB

    CBCCDCB

    9060EI3

    8EI2EI2

    60EI3

    2EI

    3

    2EI

    3

    2

    EI3

    4EI

    3

    2EI

    3

    4EI

    3

    2EI

    3

    260MMMMand

    CB

    C

    CBBDCCDBA AB

    Solving (7).(8) & (9) we get

    77.34EI

    ,18.8EI

    ,18.8EI

    C

    B

    Substituting the value of    and, CB in slope deflection equations

    KNM73.1777.343

    218.8

    3

    2M

    KNM27.1277.343

    218.8

    3

    4M

    KNM27.1218.818.85.0M

    KNM27.1218.85.018.80M

    KNM27.1277.343218.8

    34M

    KNM73.1777.343

    218.8

    3

    2M

    DC

    CD

    CB

    BC

    BA

     AB

  • 8/20/2019 Slope Def Vtu

    49/89

    Reactions: Consider the free body diagram of the members

    Member AB:

    KN103

    27.1273.17H A  

    Member BC:

    downwardsRof directionindicatessignve-KN135.6RR

    KN135.64

    27.1227.12R

    BCB

    C

  • 8/20/2019 Slope Def Vtu

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    Member CD:

    righttoleftisHof directiontheindicatessignve-KN103

    27.1273.17H DD  

    Check: ΣH = 0

    H A + HD + P = 0

    +10 + 10 – 20 = 0

    Hence okay

  • 8/20/2019 Slope Def Vtu

    51/89

    Example:  Analyse the portal frame subjected to loads as shown. Also draw

    bending moment diagram.

    The frame is symmetrical but loading is unsymmetrical. Hence there is a sway.

     Assume sway towards right. In this problem 0,0,0,0 DCB A  

    FEMs:

    KNM13.33-12

    410

    12

    wlF

    22

     AB  

    KNM13.3312

    410

    12

    wlF

    22

    BA  

    KNM112.5-8

    10908wlFBC  

    KNM112.58

    1090

    8

    wlFCB  

    Slope deflection equations:

     

      

        L

    32

    L

    EI2FM B A AB AB

    4

    30

    4

    EI213.33- B  

     

      

       

    1---------EI375.0EI5.013.33-B

     

     

      

        L

    32

    L

    EI2FM  ABBABA

    4

    302

    4

    EI213.33 B  

     

      

       

    2---------EI375.0EI13.33 B  

  • 8/20/2019 Slope Def Vtu

    52/89

    CBBCBC 2L

    EI2FM  

    210

    I3E2112.5- CB  

    3---------EI6.01.2EI112.5- CB  

    BCCBCB 2L

    EI2FM  

    210

    I3E2112.5 BC  

    4---------EI6.01.2EI112.5 BC  

     

      

        L

    32

    L

    EI2FM DCCDCD

    4

    302

    4

    EI20 C  

     

      

       

    5---------EI375.0EI C  

     

      

        L

    32

    L

    EI2FM CDDCDC

    4

    320

    4

    EI20 C  

     

      

       

    6---------EI375.00.5EI C  

    EIandEIEIunknowns3areThere CB, , accordingly the boundary conditionsare

    040HH

    0MM0MM

    D A

    CDCB

    BCBA

    4

    MMH

    MM4Hand

    4

    80MMH

    2

    4410MM4HHere

    DCCDD

    BCCDD

    BA AB A

    BA AB A

    080MMMM

    0404

    MM

    4

    80MM

    DCCDBA AB

    DCCDBA AB

  • 8/20/2019 Slope Def Vtu

    53/89

    Now MBA + MBC = 0

    (8--------0EI375.0EI6.0EI2.25.112

    0EI375.0EIEI6.0EI2.15.112

    540MMand

    (7--------017.99EI375.0EI6.0EI2.2

    0EI6.0EI2.15.112EI375.0EI33.13

    BC

    CBC

    DCCB

    CB

    CBB

    ---------080EI-1.5EI1.5EI5.1

    080EI375.0EI5.0

    EI375.0EIEI375.0EI33.13EI375.0EI5.033.13

    080MMMMalso

    CB

    C

    CBB

    DCCBBA AB

    By solving (7), (8) and (9) we get

    34.66EI

    64.59EI

    65.72EI

    C

    B

    Final moments:

    KNM70.54)34.66(375.0)64.59(5.0M

    KNM52.84)34.66(375.064.59M

    KNM52.8465.726.064.592.15.112M

    KNM10.6164.596.065.722.15.112M

    KNM10.6134.66375.065.72M

    KNM-1.8866.34375.065.725.033.13M

    DC

    CD

    CB

    BC

    BA

     AB

  • 8/20/2019 Slope Def Vtu

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    Reactions: Consider the free body diagrams of various members

    Member AB:

    lefttorightfromisHof directionindicatessignve-KN195.5

    4

    241088.110.61H

     A

     A

    Member BC:

    KN34.38R90R

    KN34.4710

    59010.6152.84R

    CB

    C

    Member CD

    KN81.344

    7.5454.84HD  

  • 8/20/2019 Slope Def Vtu

    55/89

    Check

    ΣH = 0

    H A + HD +10 × 4 = 0

    -5.20 - 34.81+ 40 = 0

    Hence okay

  • 8/20/2019 Slope Def Vtu

    56/89

    Example: Analyse the portal frame and then draw the bending moment diagram

    Solution:

    Since the columns have different moment of inertia, it is an unsymmetrical

    frame. Assume sway towards right

    FEMS:

    KNM608

    WL

    F

    KNM608

    680

    8

    WLF

    CB

    BC

    Here 0,0 D A  

    Slope deflection equations

    2--------EI8

    3EI

    4

    302

    4

    2EI0

    L32

    LEI2FM

    1--------EI8

    3EI

    2

    1

    4

    30

    4

    2EI0

    L

    32

    L

    EI2FM

    BB

     ABBABA

    BB

    B A AB AB

     

      

       

      

        

     

      

       

     

      

       

  • 8/20/2019 Slope Def Vtu

    57/89

    6---------EI4

    3EI

    4

    30

    4

    2E2I0

    L

    32

    L

    EI2FM

    5---------EI4

    3EI2

    4

    302

    4

    2E2I0

    L

    32

    L

    EI2FM

    4---------EI3

    4EI

    3

    2602

    6

    2E2I60

    2L

    EI2FM

    3---------EI3

    2EI

    3

    4602

    6

    2E2I60

    2L

    EI2FM

    CC

    CDDCDC

    CC

    DCCDCD

    CBBC

    BCCBCB

    CBCB

    CBBCBC

     

      

       

     

     

     

       

     

      

       

     

      

       

    In the above equation there are three unknowns   and, CB , accordingly theboundary conditions are,

    0MMMM

    04

    MM

    4

    MM,e.i

    conditionShear ---0HH

    conditionsintJo0MM

    0MM

    DCCDBA AB

    DCCDBA AB

    D A

    CDCB

    BCBA

    70EI8

    3EI

    3

    2EI

    3

    760

    0EI3

    2EI

    3

    460EI

    8

    3EIMM,Now

    CB

    CBBBCBA

    8060EI4

    3EI

    3

    10EI

    3

    2

    0EI4

    3EI2EI

    3

    4EI

    3

    260MM, And

    CB

    CCBCDCB

  • 8/20/2019 Slope Def Vtu

    58/89

    90EI49

    EI3EI2

    3

    EI4

    3EI

    EI4

    3EI2EI

    8

    3EIEI

    8

    3EI

    2

    1MMMM, And

    CB

    C

    CBBDCCDBC AB

    (7)inEIof valuengSubstituti

    EI3EI2

    3

    9

    4EI(9)From CB

     

      

     

    10-------060EI6

    1EI

    12

    25

    060EI2

    1EI

    4

    1EI

    3

    2EI

    3

    7

    060EI3EI2

    3

    9

    4

    8

    3EI

    3

    2EI

    3

    7

    CB

    CBCB

    CBCB

     

      

     

    Substituting value of EI in (8)

    11-------060EI3

    7EI

    6

    1

    060EIEI21EI

    310EI

    32

    060EI3EI2

    3

    9

    4

    8

    3EI

    3

    10EI

    3

    2

    CB

    CBCB

    CBCB

     

      

     

    Solving (10) & (11) we get EI B =31.03

    By Equation (11)

    3.27

    60EI6

    1

    7

    3EI BC

    Now

    55.16EI3EI2

    3

    9

    4EI CB  

     

      

     

    Now

    EI B =31.03, 3.27EI C   , EI 55.16

  • 8/20/2019 Slope Def Vtu

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    Substituting these values in slope deflection equations,The final moments are:

    KNM52.1555.164

    393.27M

    KNM45.43)55.16(4

    3)93.27(2M

    KNM43.4393.273

    403.31

    3

    260M

    KNM25.3793.273

    203.31

    3

    460M

    KNM24.3755.168

    3

    03.31M

    KNM72.2155.168

    303.31

    2

    1M

    DC

    CD

    CB

    BC

    BA

     AB

    Reactions: consider the free body diagram of beam and columns

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    Column AB:

    KN74.144

    72.2125.37H A  

    Beam BC:

    03.41R80R

    KN97.386

    38045.4325.37R

    BC

    B

    Column CD:

    KN74.144

    52.1545.43HD  

    Check:

    ΣH = 0H A + HD = 014.74-14.74=0

    Hence okay

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    Ex: Portal frame shown is fixed at ends A and D, the joint B is rigid and joint C ishinged. Analyse the frame and draw BMD.

    Solution:

    FEM’s:

    0,0,0,0,0Here

    KNM608

    680

    8

    WLF

    KNM608

    680

    8

    WLF

    CDCBBD A

    CB

    BC

    Since C is hinged member CB and CD will rotate independently. Also the

    frame is unsymmetrical, will also have sway. Let the sway be towards right.

    The slope deflections are:

    )1(EI8

    3EI

    2

    1

    4

    30

    4

    EI20

    L

    32

    L

    EI2FM

    B

    B

    B A AB AB

     

      

       

     

      

       

  • 8/20/2019 Slope Def Vtu

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    )6(EI8

    3EI

    2

    1

    4

    30

    4

    EI20

    L

    32

    L

    EI2FM

    )5(EI83EI

    4

    302

    4

    EI20

    L

    32

    L

    EI2FM

    )4(EI3

    2EI

    3

    460

    26

    I2.E260

    2

    L

    EI2FM

    )3(EI3

    2EI

    3

    460

    26

    I2.E260

    L

    32

    L

    EI2FM

    )2(EI83EI

    4

    302

    4

    EI20

    L

    32

    L

    EI2FM

    CD

    CD

    CDDDCDC

    CD

    CD

    DCDCDCD

    BCB

    BCB

    BCBCBCB

    CBB

    CBB

    CBBCBC

    B

    B

     ABBABA

     

      

       

     

      

       

     

      

       

     

      

       

     

      

       

     

      

       

     

      

       

    In the above equations areand,, CDCBB   unknowns. According theboundary conditions are

    I. MBA+MBC = 0,

    II. MCB = 0,

    III. MCD = 0,

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    IV. H A+HD = 0

    0MMMM

    04

    MM

    4

    MM,e..i

    DCCDBA AB

    DCCDBA AB

    Now using the boundary conditions:

    )14(060EI3

    2EI

    15

    26

    60EI3

    2EI

    5

    3

    3

    7

    060EI5

    8

    8

    3

    EI3

    2

    EI3

    7

    MM

    )7(EquationinngSubstituti

    )13(EI5

    8EI

    2

    3

    15

    16EIgives)12(Equation

    )12(0EI16

    15EI

    2

    3

    0EI2

    3

    EI8

    3

    2

    3

    EI2

    3

    MMMM

    )10(inSub

    )11(EI8

    3EI)9(From

    )10(0EI2

    3EI

    2

    3EI

    2

    3

    EI8

    3EI

    2

    1EI

    8

    3EIEI

    8

    3EIEI

    8

    3EI

    2

    1MMMM

    )9(0EI8

    3EIM

    )8(060EI3

    4EI

    3

    2M

    )7(060EI8

    3EI

    3

    2EI

    3

    7

    EI3

    2EI

    3

    460EI

    8

    3EIMM

    CBB

    CBB

    BCBBBCBA

    BB

    B

    BDCCDBA AB

    cD

    CDB

    CDCDBBDCCDBA AB

    CDCD

    CBBCB

    CBB

    CBBBBCBA

     

      

     

     

     

     

     

     

     

     

     

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    have we2by(14)equationgmultiplyinand)8(EquationinngSubstituti

    29.6442

    15180EI

     _  __________  __________ 

    0180EI15

    42

     _  __________  __________ 

    0120EI3

    4

    EI15

    52

    060EI3

    4EI

    3

    2

    B

    B

    CBB

    CBB

    864.10229.645

    8EI

    5

    8EIFrom(13)

    B

     

    574.38EI8

    3EI(11)From CD  

    165.77

    60864.1028

    329.64

    3

    7

    2

    3

    60EI8

    3EI

    3

    7

    2

    3EI)7(From BCB

     

      

     

     

      

     

    864.102EI,57.38EI,165.77EI,29.64EI CDCBB  

    Final Moments are

    KNM29.19864.1028

    3574.38

    2

    1M

    0864.1028

    3574.38M

    029.643

    2165.77

    3

    460M

    KNM72.25165.773

    229.64

    3

    460M

    KNM72.25864.1028

    329.64M

    KNM42.6864.1028

    329.64

    2

    1M

    DC

    CD

    CB

    BC

    BA

     AB

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    Reactions: Consider the free body diagram of various members

    Column AB:

    KN825.44

    42.672.25H A  

    Beam BC:

    KN71.3529.4480R

    KN29.446

    38072.25R

    C

    B

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    Column CD:

    KN82.44

    28.19HD  

    Check:

    ΣH = 0

    H A+HD = 0

    Hence okay.

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    Example: Analyse the portal frame shown in figure the deflection method andthen draw the bending moment diagram

    Fig

    Solution:

    The frame is unsymmetrical, hence there is a sway. Let the sway be

    towards right.

    0,0,0,0 DCB A  

    FEMS:

    KNM30215F

    KNM67.4112

    520F

    KNM67.4112

    520F

    CE

    2

    CB

    2

    BC

    Slope deflection equations

  • 8/20/2019 Slope Def Vtu

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    2--------EI375.0EI4

    302

    4

    2EI0

    L32

    LEI2FM

    1--------EI375.0EI5.04

    30

    4

    2EI0

    L

    32

    L

    EI2FM

    BB

     ABBABA

    BB

    B A AB AB

     

      

       

      

        

     

      

       

     

      

       

    6---------EI375.0EI5.04

    30

    4

    2EI0

    L

    32

    L

    EI2FM

    5---------EI375.0EI4

    302

    4

    2EI0

    L

    32

    L

    EI2FM

    4---------EI6.0EI2.167.4125

    1.5I2E67.41

    2LEI2FM

    3---------EI6.0EI2.167.4125

    1.5I2E67.41

    2L

    EI2FM

    CC

    CDDCDC

    CC

    DCCDCD

    BCBC

    BCCBCB

    CBCB

    CBBCBC

     

      

       

     

      

       

     

      

       

     

      

       

    In the above equation there are three unknowns   and, CB , accordingly theboundary conditions are,

    0MMMM,e.i

    0HH

    0MMM

    0MM

    DCCDBA AB

    D A

    CECDCB

    BCBA

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    Now,

    7067.41EI375.0EI6.0EI2.20EI6.0EI2.167.141EI375.0EI

    0MM

    CB

    CBB

    BCBA

    8067.11EI375.0EI2.2EI6.0030EI375.0EIEI6.0EI2.167.41MM, And

    CB

    CBCCDCB

    90EI5.1EI5.1EI5.1

    0EI375.0EI5.0EI375.0EI2EI375.0EIEI375.0EI5.0

    0MMMM

    CB

    CCBB

    DCCDBC AB

    Solving the above equationswe get, EI 98.23B   , EI 62.14EI,36.9C  

    Substituting these values in slope deflection equations, we have

    KNM30MKNM16.1062.14375.036.95.0M

    KNM84.14)62.14(375.036.9M

    KNM83.4498.236.036.92.167.41M

    KNM51.1836.96.098.232.167.41M

    KNM50.1862.14375.098.23M

    KNM50.662.14375.098.235.0M

    CE

    DC

    CD

    CB

    BC

    BA

     AB

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    Reactions: consider the free body diagram of beam and columns

    Column AB:

    KN25.64

    5.65.18H A  

    Span BC:

    73.44R520R

    KN27.555

    5.25205.1883.44R

    CB

    C

    Column CD:

    25.64

    84.1416.10HD  

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    Check:

    ΣH = 0H A + HD = 0Σ = 0

    Hence okay

  • 8/20/2019 Slope Def Vtu

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    Example: Analyse the portal frame shown and then draw bending momentdiagram.

    Solution:

    It is an unsymmetrical problem hence there is a sway be towards right

    0,0,0,0 DCB A  

    FEMs:

    KNM41.67-12

    520

    12

    wlF

    22

    BC  

    KNM41.6712

    520

    12

    wl

    F

    22

    CB  

    Slope deflection equations:

     

      

        L

    32

    L

    EI2FM B A AB AB

    3

    30

    3

    EI20 B  

     

      

       

    1---------EI3

    2EI

    3

    2B  

           L32

    LEI2FM  ABBABA

    3

    302

    3

    EI20 B  

     

      

       

    2---------EI3

    2EI

    3

    4B  

  • 8/20/2019 Slope Def Vtu

    73/89

     

      

        L

    32

    L

    EI2FM CBBCBC

    25

    I5.1E241.67- CB  

    3---------EI53

    EI5

    641.67- CB  

     

      

       

    L

    32

    L

    EI2FM BCCBCB

    025

    I5.1E267.41 BC  

    4---------EI6.01.2EI41.67 BC  

     

      

       

    L

    32

    L

    EI2FM DCCDCD

    4

    3

    024

    EI2

    0 C    

     

     

       

    5----------EI375.0EI C  

     

      

        L

    32

    L

    EI2FM CDDCDC

    4

    30

    4

    EI20 C  

     

      

       

    6----------EI375.00.5EI C   In the above equations there are three unknown   and, CB and accordingly theBoundary conditions are:

    0)MM(3)M4(M

    04

    MM

    3

    MMi.e

    0HH

    0MM

    0MM

    DCCDBA AB

    DCCDBA AB

    D A

    CDCB

    BCBA

  • 8/20/2019 Slope Def Vtu

    74/89

    Now

    )8(0EI375.0EI6.0EI2.267.41

    0EI375.0EIEI6.0EI2.167.41

    0MM

    )7(067.41EI3

    2EI5

    3EI53.2

    67.41EI5

    3EI

    5

    6EI

    3

    2EI

    3

    4

    0MM

    BC

    CBC

    CDCB

    CB

    CBB

    BCBA

    04

    MM

    3

    MM DCCDBA AB

    )9(0EI53.7EI5.4EI8

    0EI25.2EI5.4EI3

    8EI

    3

    16EI

    3

    8EI

    3

    80EI375.0EI5.0EI375.0EI3

    EI3

    2EI

    3

    4EI

    3

    2EI

    3

    24

    CB

    CBB

    CC

    BB

    By solving (7), (8) and (9) we get

    8.12EI

    17.23EI

    46.25EI

    C

    B

    Final moments:

    KNM65.1680.12375.070.235.0M

    KNM50.28)80.12(375.070.23M

    KNM50.2846.2060.017.232.167.41M

    KNM40.2567.4117.235

    346.25

    5

    6M

    MKN40.258.123

    246.25

    3

    4M

    KNM8.448.123

    246.25

    3

    2M

    DC

    CD

    CB

    BC

    BA

     AB

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    Reactions: Consider the free body diagram

    Member AB:

    KN28.113

    44.840.25H A  

  • 8/20/2019 Slope Def Vtu

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    Member BC:

    KN36.4864.51520R

    KN64.512

    2

    552030.205.28

    R

    B

    C

    Member CD:

    HD =4

    65.165.28   = 11.28 KN

    Check:

    ΣH = 0H A + HD = 0Satisfied, hence okay

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    Example: A portal frame having different column heights are subjected for forces

    as shown in figure. Analyse the frame and draw bending moment diagram.

    Solution:-

    It is an unsymmetrical problem

    0,0,0,0 DCB A   , hence there is a sway be towards right.

    FEMs:

    KNM15-8

    430

    8

    WlF AB  

    KNM158

    430

    8

    WlFBA  

    KNM30-8

    460

    8

    WlFBC  

    KNM308

    460

    8

    WlFCB  

    CDF = DCF = 0

    Slope deflection equations:

     

      

       

    L

    32

    L

    EI2FM B A AB AB

    4

    30

    4

    I2E215- B  

     

      

       

    1--------EI75.0EI15- B  

  • 8/20/2019 Slope Def Vtu

    78/89

     

      

       

    L

    32

    L

    EI2FM  ABBABA

    4

    302

    4

    I2E215 B  

     

      

       

    2--------EI75.0EI215 B  

    CBBCBC 2L

    EI2FM  

    24

    I2E230- CB  

    3---------EIEI230- CB  

    BCCBCB 2L

    EI2FM  

    24

    I2E230 BC  

    4---------EI2EI30 BC  

     

      

       

    L

    32

    L

    EI2FM DCCDCD

    3

    302

    3

    EI20 C  

     

      

       

    5---------EI

    3

    2EI

    3

    4

    C

     

     

      

       

    L

    32

    L

    EI2FM CDDCDC

    3

    30

    3

    EI20 C  

     

      

       

    6---------EI3

    2EI

    3

    2C  

    There are three unknowns, EI,   EI&EI, CB , accordingly the Boundaryconditions are

  • 8/20/2019 Slope Def Vtu

    79/89

    0180MM4MM3

    030

    3

    MM

    4

    60MM,e.i

    030HH

    0MM

    0MM

    DCCDBA AB

    DCCDBA AB

    D A

    CDCB

    BCBA

    Now

    7015EI75.0EIEI4EIEI230EI75.0EI215MM

    CB

    CBBBCBA

    8030EI

    3

    2EI

    3

    10EI

    EI3

    2EI

    3

    4EIEI230MM

    CB

    CBCCDCB

    90180EI833.9EI8EI9

    180EI3

    2EI

    3

    2EI

    3

    2EI

    3

    44

    EI75.0EI215EI75.0EI153180)MM(4)MM(3

    CB

    CC

    BBDCCDBA AB

     

      

     

    By solving (7), (8) & (9) we get

    795.20EI

    714.7EI

    577.9EI

    C

    B

    Substituting these values in the slope deflection equations we get

    KNM00.19795.203

    2)714.7(

    3

    2M

    KNM15.24795.20

    3

    2)714.7(

    3

    4M

    KNM15.24577.9714.7230M

    KNM18.55-7.714-9.577230-M

    KNM55.18795.2075.0577.9215M

    KNM01.21795.2075.0577.915M

    DC

    CD

    CB

    BC

    BA

     AB

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    Reactions: Consider free body diagrams of the members

    Member AB:

    KN615.154

    23001.2155.18H A  

    -ve sign indicates the direction of H A is from right to left.

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    Member BC:

    KN40.3160.28R60R

    KN60.284

    15.2426055.18R

    BC

    B

    Member CD:

    KN38.143

    15.2419HD  

    Check:ΣH = 0

    H A + HD + 30 = 0

    -15.62 – 14.38 + 30 = 0

    Hence okay

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    Example:  Analyse the frame using slope deflection method and draw the

    Bending Moment Diagram.

    Solution:  Assume sway towards right

  • 8/20/2019 Slope Def Vtu

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    It can be observed from figure in that direction of moments due to sway in

    member AB are anticlockwise and that for member CD are clockwise. Wise shall

    be taken to incorporate the same in the slope deflection equation.

    FEMS

    0Here

    MKN3212

    wIF

    MKN3212

    424-

    12

    wIF

    D A

    2

    CB

    2

    2

    BC

    Slope deflection equations are:

    2EI3

    2EI

    3

    4

    3

    32

    3

    EI2

    L

    32

    L

    EI2FM

    1-------EI3

    2EI

    3

    23

    3

    3

    EI2

    L

    32

    L

    EI2FM

    B

    B

     ABBABA

    B

    B

    B A AB AB

     

      

       

     

      

       

     

     

     

       

     

      

       

  • 8/20/2019 Slope Def Vtu

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    5EI3

    2EI

    3

    43

    32

    3

    2EI

    L

    32

    L

    EI2FM

    4--------EIEI232

    24

    I2E232

    2L

    EI2FM

    3---------EIEI232

    24

    I2E232

    2L

    EI2FM

    C

    C

    DCCDCD

    BC

    BC

    BCCBCB

    CB

    CB

    CBBCBC

     

     

      

       

    6--------EI3

    2EI

    3

    2

    3

    3

    3

    EI2

    L

    32

    L

    EI2FM

    C

    C

    CDDCDC

     

      

       

     

    The unknown are &, C,B   areconditionsboundarythey Accordingl

    090MMMM

    0303

    MM

    3

    MM,e.i

    030HH

    0MM

    0MM

    DCCDBA AB

    DCCDBA AB

    D A

    CDCB

    BCBA

    7032EI3

    2EIEI

    3

    10

    EIEI232EI3

    2EI

    3

    4MM,Now

    CB

    CBBBCBA

  • 8/20/2019 Slope Def Vtu

    85/89

    8032EI3

    2EI

    3

    10EI

    EI3

    2EI

    3

    4EIEI232MM

    CB

    CBCCDCB

    9045EI3

    4EIEI

    90EI3

    8EI2EI2

    90EI3

    2EI

    3

    2EI

    3

    2

    EI3

    4EI

    3

    2EI

    3

    4EI

    3

    2EI

    3

    290MMMM

    CB

    CB

    C

    CBBDCCDBA AB

    From (7) & (9)

    10-------0109EI3EI3

    17

    045EI3

    4EIEI

    064EI3

    4EI2EI

    3

    20

    CB

    CB

    CB

    By (8) and (9)

    11--------0109EI3

    17EI3

    045EI3

    4EIEI

    064EI3

    4

    EI3

    20

    EI2

    CB

    CB

    CB

    By (10) & (11)

    071.166EI317

    208

    071.57EI3EI

    17

    27

    0109EI3EI3

    17

    B

    CB

    CB

    88.40208

    31771.166EI B  

  • 8/20/2019 Slope Def Vtu

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    From (10)

    88.40EI3

    17109

    3

    1EI BC  

    From (9)

    07.954588.4088.404

    3

    45EIEI4

    3

    EI CB

    Thus 07.95EI,88.40EI,88.40EI CB  

    Substituting these values in slope deflection equations

    KNM12.3607.953

    288.40

    3

    2M

    KNM88.807.953

    288.40

    3

    4M

    KNM88.888.4088.40232M

    KNM88.888.4088.40232M

    KNM88.807.95

    3

    288.40

    3

    4M

    KNM12.3607.953

    288.40

    3

    2M

    DC

    CD

    CB

    BC

    BA

     AB

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    To find the reaction consider the free body diagram of the frame

    Reactions:

    Column AB

    KN153

    12.3688.8H A  

    Beam AB

    KN484

    2

    442488.888.8

    RB  

    KN4848424R

    Column CD

    KN153

    12.3688.8HD  

  • 8/20/2019 Slope Def Vtu

    88/89

    CheckΣH = 0H A + HD +P = 0

    -15 – 15 + 30 = 0Hence okay

  • 8/20/2019 Slope Def Vtu

    89/89