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Unit - 5


Slope defection method as applied to indeterminate beams


1. Slope Deflection Method

  • Slope=
  • Deflection=
  • Sign Convention
  1. Simply supported Beam

 

At support form

At the simply supported end

is always zero.

is always zero.

 

2.     Cantilever beam

 

1. =0 at the fixed end at force end

At Fixed end

 

2. Slope deflection equation:

When a member of a structure is loaded, it deforms from its original position and internal forces are developed. The end moments can be expressed in terms of

(i)                Fixed end moments (FEM) of the member due to transverse loading on the member

(ii)              The slopes or rotations at the end

(iii)           The end deflections or joint translations. These expressions are called as Slope-Deflection equations.

There are two slope deflection equations for each member.

These slope deflection equations are derived from superposition of the end moments caused by various actions and displacement.

Similarly

Where,

= be the slope or rotation at joint A

= be the slope or rotation at joint B.

= be the end deflection or translation of joint A.

= be the end deflection or translation of joint B.

B/A = Relative translation of joint B with respect to joint A

AB Angle between the unreformed member and the line joining the deflected joints.

Here > Therefore B/A is positive

MAB = Moment at A of member AB

МВА = Moment at B of member BA

 

3. Fixed End Moments: Standard Cases Fixed End Moments

Standard Cases

1.

 

2.

 

3.

 

4.

 

5.

 

4. Derivation of slope Deflection Method

  • In beam, a continuous beam ABCD, consider AB part and take fixed end moments and rotation at support as given below

 

As per the diagram

Slop deflection equations are

.

5.  Types of numerical for slope deflection method

1. The beam is without sink (is zero.)

2. Beam with sink (is given)

3. Analyze of the frame without sink

4. Analyze the frame with the sink.

 

6. Steps for analysis of the slope deflection method

1. Find unknown slope.

2. Find fixed end moment

3. Apply the slope deflection equation.

4. Use the joint equilibrium equation at the joint.

5. Find final moments.

6. Find relation by equation &Draw SFI

7. Draw BMD

 

Hod

 

Step-III Apply equilibrium condition at joint

 

Step-IV   Find final moments.

 

Step-V Find reaction

S.F. At A Take a moment at A is

 

SFD & BMD

 

  1. Determine support moments & draw BMD for the beam shown by using S.D.

 

Step-I) Find Dki

 

Step II) Find fixed end moments

For BC Beam

 

 

Step-III) Apply the SD equation

AB=>

BC=>

 

Step- IV) Apply equilibrium condition joint B

-------   due to Hinge support

Put in equation (1) (2) (3) & (4)

 

Draw BMD Diagram

 

2.     Analyze the continuous beam ABCD by S.D. Method draw BMD

 

Modify Diagram

 

Step- I) Fixed end moment

 

Apply S.D. Equation

Member BC

Member CD

 

Step 4) To apply condition of equilibrium

At joint B

Adding equation 1and 2

Due to symmetry

 

Step 5) To find end moments at joint

 

Step 6) Draw BMD and SFD

 

 

SFD

 

BMD

 


C:\Users\TARUNA\Desktop\internship\february\11 feb2020\last\5.JPG

 

∑MA = MA – (10+Q)(1) = 0

MA = 10 + Q

∑F y = VA – (10 + Q) = 0 VA = 10 + Q

∑F x = HA = 0

C:\Users\TARUNA\Desktop\internship\february\11 feb2020\last\4.JPG

 

Zone    origin       limits         EI            M                 ӘM/ӘQ

AB               A                     0 – 2                2EI       (10+Q) x-(10+Q)       x-1

CB              C                     0 – 1                EI          - (10 + Q)                    -1

DC              D                    0 – 1                 EI          - (10 + Q) x                 - x

 

Δ D y = ∫20 (10x - 10)(x-1)dx/2EI + ∫10 -10(-1)dx/EI + ∫10 -10x(-x)dx/EI

= 3.33 + 10 + 3.33/EI

Δ D y   = 16.66/EI (       )

 


1. Portal method

This method is applicable for low rise structures. In low rise structures shear deformations are dominant, therefore this method simplifying assumptions regarding horizontal shear in column. Each bay of a structure as a portal frame and horizontal force is distributed equally among them. This means each interior column takes twice as much as the exterior column

 

Assumptions:

  1. The points of inflection or point of contra flexure are located at the mid height of each column. However for hinged column base it assumed at hinged column base
  2. The point of inflection are located at mid span of beam
  3. The horizontal shear at any floor is divided among all the basis that each interior column take twice as much as the exterior column

 

Steps

1)     Assume first assumption -> mark point of contra flexure at centre of each column & beam

2)     Apply 2nd assumption -> Horizontal shear is double at interior column.

3)     Find P& Q force.

4)     Find moment at beam = always same as moment of column.

5)     Find shear force at beam=moment at

 

Problems:

1)     Analyse the given figure by portal method

 

Step 1) 1st Assumption-> Mark point of contraflexure of each member

 

Step 2) 2nd Assumption -> Interior Horizontal shear is double than (extreme) lost member.

P+2P+P=12

P=3KN

Q+2Q+Q=12+24

Q=9KN

 

Step 3) Moment at the end of column

 

Step 4) Moment at column

 

Step5) Moment at the end of roof Beam

 

Step 6) Moment at the end of floor Beam

 

Step 7) Shear force in Beam

Similarly,

 

  1. Analyse the given figure by portal Method

Mark point of contra flexure at centre of each beam& column.

Horizontal share is double at interior column.

Find p & q

P+2P+P=20

P=5kN

Q +2Q +Q=50

Q=12.5KN

Moment at column AD= =

MBE=

MCF=

MDG=MGD=

MEH=MHE=

MFI=MIF=

 

2.     Analyse the given figure by portal method

P+2P+2P+P=25

4P=25

P=4.16

Q+2Q+2Q+Q=60

6Q=60

Q=10KN

MAE=MEA==4.16

MBF=MFB=

MCG=MGC=

MDH=MHD=

MEI=MIE==10

MFI=MIF=

MGK=MKG=

MHL=MLH=

 

Shear force

SFAB=20.8/2=10.4

SFBC=20.8/3=6.93

SFCD=20.8/4=5.2

SFEF=60.8/2=30.4

SFFG=60.8/3=20.26

SFGH=60.8/4=15.3

 

BMD

 

3.     Analyze the given figure by portal method

P=3.33      Q=3.33     R=10

 

4.     Analyze the frame shown in figure below by portal method

 

1) Apply 1st assumption

2) Apply 2nd Assumption-> Horizontal shear is double at interior member

P+2p+p=25

P=6.25KN

Q+2Q+Q=25+50

Q=18.75KN

3) Moment at the end of column

4) Moment at the end of floor column

5) Moment at beam

6)Moment at end of beam

7)Shear force at (beam) floor

 

  1. Cantilever Method

The cantilever method is based on the following assumption:

Assumption

  1. There is a point of contraflexure at the centre of each member.
  2. The intensity of axial stress in each column storey is proportional to the horizontal distribution of that column from the centre of gravity of all columns of the storey under consideration.

 

Application:

  1. The method is more applicable to high rise structure since bending action is more predominant in these cases
  2. The column having different area of cross section can be taken into account.

 

Problem:

  1. Determine the approximate value of bending moment shearing force and axial force in a two bay two storey portal portal frame shown in fig. Using cantilever method assume equal cross sectional areas for all columns

 

Step-1 Find centroidal distance

Take moment about A

 

Step-2>As per 2nd assumption

Vertical stresses in column are proportional to their absence from the C.G. Of the columns in that storey.

1>  Consider top storey

Assume is downward & is upward.

Put values

Taken about point of contra flexure i.e. at 0 point

Clockwise +ve               Anticlockwise  -ve

Upward      +ve                Downward       -ve

Consider lowest storey

Assume are downward

are upward

 

As per 2nd assumption

Take a moment about 0 point.

 

Step-3) To find S.F. In proof Beam

S.F. In AB=1KN

SF in BC=1+0.42=1.42

SF in CD=1+0.42-0.28=1.14

S.F. In EF=6-1=5KN

S.F. In FG=6+2.57+1-0.48=7.15KN

SF in GH=6+2.37-1.71-1-1-0.42+0.28=5.72KN

 

Step-4) To find Moment in roof beam

Formula => Moment in roof beam=S.F. In that Beam*Balt of Beam span

Ii> To find moment in floor beam

 

Step -5) To find Moment in column

Moment in column of floor beam

 

Step-6) S.F. In column

S.F. AE=2/1.5=1.33KNM

SF BF=5.55/1.5=3.7KN

S.F. CG=6.9/1.5=4.6KN

S.F. DH=3.42/1.5=2.28KN

S.F. In column EI=1.33*1.5+x+2=10

X=4KN

S.F. In column FJ=3.725*1.5+x+2=(17.85+10)

X=11.128KN

S.F. In column GK=4.667*1.5+x*2=(17.14+17.85)

X=13.99KN

S.F. In column HL=2.28*1.5+x+2=(17.142)

X=6.86KN

 

Key takeaways:

Steps:

  1. Find centroidal distance
  2. As per 2nd assumption
  3. To find S.F. In proof Beam
  4. To find Moment in roof beam
  5. To find Moment in column
  6. S.F. In column

 

References:

1. Structural Analysis by C.S. Reddy Mc. Graw Hill

2. Structural Analysis by R.C. Hibbler Pearson Education



Unit - 5


Slope defection method as applied to indeterminate beams



Unit - 5


Slope defection method as applied to indeterminate beams


1. Slope Deflection Method

  • Slope=
  • Deflection=
  • Sign Convention
  1. Simply supported Beam

 

At support form

At the simply supported end

is always zero.

is always zero.

 

2.     Cantilever beam

 

1. =0 at the fixed end at force end

At Fixed end

 

2. Slope deflection equation:

When a member of a structure is loaded, it deforms from its original position and internal forces are developed. The end moments can be expressed in terms of

(i)                Fixed end moments (FEM) of the member due to transverse loading on the member

(ii)              The slopes or rotations at the end

(iii)           The end deflections or joint translations. These expressions are called as Slope-Deflection equations.

There are two slope deflection equations for each member.

These slope deflection equations are derived from superposition of the end moments caused by various actions and displacement.

Similarly

Where,

= be the slope or rotation at joint A

= be the slope or rotation at joint B.

= be the end deflection or translation of joint A.

= be the end deflection or translation of joint B.

B/A = Relative translation of joint B with respect to joint A

AB Angle between the unreformed member and the line joining the deflected joints.

Here > Therefore B/A is positive

MAB = Moment at A of member AB

МВА = Moment at B of member BA

 

3. Fixed End Moments: Standard Cases Fixed End Moments

Standard Cases

1.

 

2.

 

3.

 

4.

 

5.

 

4. Derivation of slope Deflection Method

  • In beam, a continuous beam ABCD, consider AB part and take fixed end moments and rotation at support as given below

 

As per the diagram

Slop deflection equations are

.

5.  Types of numerical for slope deflection method

1. The beam is without sink (is zero.)

2. Beam with sink (is given)

3. Analyze of the frame without sink

4. Analyze the frame with the sink.

 

6. Steps for analysis of the slope deflection method

1. Find unknown slope.

2. Find fixed end moment

3. Apply the slope deflection equation.

4. Use the joint equilibrium equation at the joint.

5. Find final moments.

6. Find relation by equation &Draw SFI

7. Draw BMD

 

Hod

 

Step-III Apply equilibrium condition at joint

 

Step-IV   Find final moments.

 

Step-V Find reaction

S.F. At A Take a moment at A is

 

SFD & BMD

 

  1. Determine support moments & draw BMD for the beam shown by using S.D.

 

Step-I) Find Dki

 

Step II) Find fixed end moments

For BC Beam

 

 

Step-III) Apply the SD equation

AB=>

BC=>

 

Step- IV) Apply equilibrium condition joint B

-------   due to Hinge support

Put in equation (1) (2) (3) & (4)

 

Draw BMD Diagram

 

2.     Analyze the continuous beam ABCD by S.D. Method draw BMD

 

Modify Diagram

 

Step- I) Fixed end moment

 

Apply S.D. Equation

Member BC

Member CD

 

Step 4) To apply condition of equilibrium

At joint B

Adding equation 1and 2

Due to symmetry

 

Step 5) To find end moments at joint

 

Step 6) Draw BMD and SFD

 

 

SFD

 

BMD

 


C:\Users\TARUNA\Desktop\internship\february\11 feb2020\last\5.JPG

 

∑MA = MA – (10+Q)(1) = 0

MA = 10 + Q

∑F y = VA – (10 + Q) = 0 VA = 10 + Q

∑F x = HA = 0

C:\Users\TARUNA\Desktop\internship\february\11 feb2020\last\4.JPG

 

Zone    origin       limits         EI            M                 ӘM/ӘQ

AB               A                     0 – 2                2EI       (10+Q) x-(10+Q)       x-1

CB              C                     0 – 1                EI          - (10 + Q)                    -1

DC              D                    0 – 1                 EI          - (10 + Q) x                 - x

 

Δ D y = ∫20 (10x - 10)(x-1)dx/2EI + ∫10 -10(-1)dx/EI + ∫10 -10x(-x)dx/EI

= 3.33 + 10 + 3.33/EI

Δ D y   = 16.66/EI (       )

 


1. Portal method

This method is applicable for low rise structures. In low rise structures shear deformations are dominant, therefore this method simplifying assumptions regarding horizontal shear in column. Each bay of a structure as a portal frame and horizontal force is distributed equally among them. This means each interior column takes twice as much as the exterior column

 

Assumptions:

  1. The points of inflection or point of contra flexure are located at the mid height of each column. However for hinged column base it assumed at hinged column base
  2. The point of inflection are located at mid span of beam
  3. The horizontal shear at any floor is divided among all the basis that each interior column take twice as much as the exterior column

 

Steps

1)     Assume first assumption -> mark point of contra flexure at centre of each column & beam

2)     Apply 2nd assumption -> Horizontal shear is double at interior column.

3)     Find P& Q force.

4)     Find moment at beam = always same as moment of column.

5)     Find shear force at beam=moment at

 

Problems:

1)     Analyse the given figure by portal method

 

Step 1) 1st Assumption-> Mark point of contraflexure of each member

 

Step 2) 2nd Assumption -> Interior Horizontal shear is double than (extreme) lost member.

P+2P+P=12

P=3KN

Q+2Q+Q=12+24

Q=9KN

 

Step 3) Moment at the end of column

 

Step 4) Moment at column

 

Step5) Moment at the end of roof Beam

 

Step 6) Moment at the end of floor Beam

 

Step 7) Shear force in Beam

Similarly,

 

  1. Analyse the given figure by portal Method

Mark point of contra flexure at centre of each beam& column.

Horizontal share is double at interior column.

Find p & q

P+2P+P=20

P=5kN

Q +2Q +Q=50

Q=12.5KN

Moment at column AD= =

MBE=

MCF=

MDG=MGD=

MEH=MHE=

MFI=MIF=

 

2.     Analyse the given figure by portal method

P+2P+2P+P=25

4P=25

P=4.16

Q+2Q+2Q+Q=60

6Q=60

Q=10KN

MAE=MEA==4.16

MBF=MFB=

MCG=MGC=

MDH=MHD=

MEI=MIE==10

MFI=MIF=

MGK=MKG=

MHL=MLH=

 

Shear force

SFAB=20.8/2=10.4

SFBC=20.8/3=6.93

SFCD=20.8/4=5.2

SFEF=60.8/2=30.4

SFFG=60.8/3=20.26

SFGH=60.8/4=15.3

 

BMD

 

3.     Analyze the given figure by portal method

P=3.33      Q=3.33     R=10

 

4.     Analyze the frame shown in figure below by portal method

 

1) Apply 1st assumption

2) Apply 2nd Assumption-> Horizontal shear is double at interior member

P+2p+p=25

P=6.25KN

Q+2Q+Q=25+50

Q=18.75KN

3) Moment at the end of column

4) Moment at the end of floor column

5) Moment at beam

6)Moment at end of beam

7)Shear force at (beam) floor

 

  1. Cantilever Method

The cantilever method is based on the following assumption:

Assumption

  1. There is a point of contraflexure at the centre of each member.
  2. The intensity of axial stress in each column storey is proportional to the horizontal distribution of that column from the centre of gravity of all columns of the storey under consideration.

 

Application:

  1. The method is more applicable to high rise structure since bending action is more predominant in these cases
  2. The column having different area of cross section can be taken into account.

 

Problem:

  1. Determine the approximate value of bending moment shearing force and axial force in a two bay two storey portal portal frame shown in fig. Using cantilever method assume equal cross sectional areas for all columns

 

Step-1 Find centroidal distance

Take moment about A

 

Step-2>As per 2nd assumption

Vertical stresses in column are proportional to their absence from the C.G. Of the columns in that storey.

1>  Consider top storey

Assume is downward & is upward.

Put values

Taken about point of contra flexure i.e. at 0 point

Clockwise +ve               Anticlockwise  -ve

Upward      +ve                Downward       -ve

Consider lowest storey

Assume are downward

are upward

 

As per 2nd assumption

Take a moment about 0 point.

 

Step-3) To find S.F. In proof Beam

S.F. In AB=1KN

SF in BC=1+0.42=1.42

SF in CD=1+0.42-0.28=1.14

S.F. In EF=6-1=5KN

S.F. In FG=6+2.57+1-0.48=7.15KN

SF in GH=6+2.37-1.71-1-1-0.42+0.28=5.72KN

 

Step-4) To find Moment in roof beam

Formula => Moment in roof beam=S.F. In that Beam*Balt of Beam span

Ii> To find moment in floor beam

 

Step -5) To find Moment in column

Moment in column of floor beam

 

Step-6) S.F. In column

S.F. AE=2/1.5=1.33KNM

SF BF=5.55/1.5=3.7KN

S.F. CG=6.9/1.5=4.6KN

S.F. DH=3.42/1.5=2.28KN

S.F. In column EI=1.33*1.5+x+2=10

X=4KN

S.F. In column FJ=3.725*1.5+x+2=(17.85+10)

X=11.128KN

S.F. In column GK=4.667*1.5+x*2=(17.14+17.85)

X=13.99KN

S.F. In column HL=2.28*1.5+x+2=(17.142)

X=6.86KN

 

Key takeaways:

Steps:

  1. Find centroidal distance
  2. As per 2nd assumption
  3. To find S.F. In proof Beam
  4. To find Moment in roof beam
  5. To find Moment in column
  6. S.F. In column

 

References:

1. Structural Analysis by C.S. Reddy Mc. Graw Hill

2. Structural Analysis by R.C. Hibbler Pearson Education


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