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REVIEW OF 
BASIC 
STRUCTURAL 
ANALYSIS 
PRESENTED BY: 
HASSAN ABBA MUSA 
1401306006
#1 - INTRODUCTION TO STRUCTURAL 
ANALYSIS 
Structural Analysis is the analysis of a given structure 
subject to some given loads, and the idea is to predict the 
response of the structure (system), thus there are some 
inputs referred to as ‘’stimulus’’ and an outputs referred to 
as ‘’response’’. The Structural analysis is the application 
of solid mechanics to predict the response (Interms of 
forces & displacements) of a given structure (existing or 
proposed) that subjected to a specified loads. 
LOADS 
(INPUTS) 
RESPONSE 
(INPUTS) 
STRUCTURE (SYSTEM)
Loads are classified into 2 parts: 
 Dead loads (Self-weight; of the components of the 
structure). 
 Imposed loads & forces (Live, Wind, Snow, Rain, and 
Temperature, Erection loads, Seismic forces & others). 
The Structural Analysis is only ascertained correct 
when the following requirements were satisfied;- 
 Equilibrium Forces. 
 Compatibility of Displacement. 
 Force/Displacement Relations. 
Therefore, In every forms of the structures, the 
structural Engineer has to consider the following 
structural considerations and purposes.
 Stability, 
 Strengths, 
 Stiffness, 
 Economy, as well as 
 Aesthetic aspects of the structure. 
The following Softwares are available 
 Orion, 
 STAAD III, 
 ANSYS, 
 AXIS VM, 
 ETABS, SAP, Etc
#2 – DIFFERENT TYPES OF SUPPORTS 
 Roller, 
 Pinned, 
 Hinged, 
 Fixed, 
 Link, 
 Ball and Socket, 
 Rigid Support, 
 Spring Support. 
FORCES
#2 – DIFFERENT TYPES OF STRUCTURES 
 Frame Structure, 
 Truss Structure, 
 Shell Structure, 
 Arch Structure, 
 Suspension Structure, 
 Mass Structure, & 
 Composite Structure.
#3 – LIST OF EQUILIBRIUM EQUATIONS 
For state of static equilibrium to exist, it is necessary that the 
combined resultant effect of the system of forces shall be neither 
a Force nor a Couple; otherwise there will be tendency for 
motion of a body. However, many 3D structures are idealized as 
series of 2D components: 
 If the combined resultant effect of a general system of forces 
acting on a planar structures is not be equivalent to a resultant 
force, the algebraic sum of all F푥 components must be equal to 
Zero and the algebraic sum of all F푦 components must to be 
equal to Zero, i.e F푥 = 0 F푦 = 0. 
 If the combined resultant effect is not to be equivalent to a 
couple, the algebraic sum of the moment M푧 of all forces 
about any axis parallel to the Z-reference axis and normal to 
the plane of the structure must be equal to zero, i.e M푧 = 0 .
#4 – DETERMINATE AND INDETERMINATE 
OF A STRUCTURE 
If the number of unknown forces is identical to the 
number of equilibrium equations, the problem is said to 
be Statically Determinate since the unknown forces can 
be determined directly from the equilibrium. 
2푗 = 푚 + 푟 푤ℎ푒푟푒 푛 = 0 
If, however the number of unknown forces exceeds the 
number of equilibrium equations, the problem is said to 
be Statically Indeterminate to a degree equal to this 
excess. 
2푗 > 푚 + 푟 푤ℎ푒푟푒 푛 ≠ 0 
푗 = 푁표. 표푓 푗표푖푛푡푠, 푚 = 푁표. 표푓 푚푒푚푏푒푟푠, 
푟 = 푁표. 표푓 푟푒푎푐푡푖표푛푠
#5 – TECHNIQUES USED IN ANALYSING 
STRUCTURE 
 Macaulay’s Method 
 Moment Area Method 
 Conjugate Beam Method 
 Virtual Work Method 
 Unit load Method 
 Influence line theory 
 The Three Moment Equation (Clapeyron’s Theorem) 
 Stiffness & Flexibility Method 
 Slope Deflection Method 
 Moment Distribution Method
MACAULAY’S METHOD 
This is a method suggested by W. H. Macaulay to relate 
the stiffness, radius of curvature, deflection and the 
bending moments in a beam by integration methods. 
Beam Deflections using successive integration; 
Consider an infinitely small 
Section, dx, of the above loaded 
beam;
MOMENT AREA METHOD 
 This is a method suitable for calculating slope & 
deflection at selected points on a beam. 
 It is also effective for calculating the deflections of 
beams with various cross sections. 
 The simplest way to evaluate the fixed -end moments, 
etc, will often be by the use of the Moment area method. 
There are two theorems associated with the moment area 
methods: 
First Moment Area Theorem: 
“The difference in slope between two points on a beam is 
equal to the area of the M/EI diagram between the two 
points.”
Second Moment Area Theorem: 
“The moment about a point A of the M/EI diagram between 
points A and B will give the deflection of point A relative 
to the tangent at point B.” 
First Moment Area Theorem 
Second Moment Area 
Theorem
#6 – INTRODUCTION TO 
FLEXIBILITY/STIFFNESS METHOD 
Flexibility Method (Force Method of Analysis) 
In this method, the degree of statical indeterminacy is 
initially determined. Thereafter, a number of releases equal to 
the degree of statical indeterminacy is introduced, each 
release being made by the removal of an external or internal 
force. Hence, the forces on the original indeterminate 
structure are calculated as the sum of the correction forces 
(redundants) and forces on the released structure. Flexibility 
Matrix [ f] ;- [f]{F} = {Δ − 퐷} 
D represents inconsistencies in deformation while {F} 
represents the redundants, Δ Elements represent prescribed 
displacements at their respective coordinates. The column 
vector {Δ - D} thus depends on the external loading.
Stiffness Method (Displacement Method of Analysis) 
The displacement method can be applied to statically determinate 
or indeterminate structures, but is more useful in the latter, 
particularly when the degree of statical indeterminacy is high. 
In this method, one must first determine the degree of kinematic 
indeterminacy. A coordinate system is then established to identify 
the location and direction of joint displacements. Restraining 
forces equal in number to the degree of kinematic indeterminacy 
are introduced at the co-ordinates to prevent the displacement of 
the joints. Stiffness Matrix [S];- 
{D} = [푆]−1{-F} 
The elements of the vector {D} are the unknown displacements. 
The elements of the matrix [S] are forces corresponding to unit 
values of displacements. 
The column vector {F} depends on the loading on the structure.
#3 – MATRIX OPERATIONS 
Let A, B, and C be mxn matrices. We have 
Properties involving Addition. 
1. A+B = B+A 
2. (A+B)+C = A + (B+C) 
3. A+0 = A where is the mx zero-matrix (all its entries 
are equal to 0); 
4. A+B = 0, if and only if B = -A.

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Review of Basic Structural Analysis Techniques

  • 1. REVIEW OF BASIC STRUCTURAL ANALYSIS PRESENTED BY: HASSAN ABBA MUSA 1401306006
  • 2. #1 - INTRODUCTION TO STRUCTURAL ANALYSIS Structural Analysis is the analysis of a given structure subject to some given loads, and the idea is to predict the response of the structure (system), thus there are some inputs referred to as ‘’stimulus’’ and an outputs referred to as ‘’response’’. The Structural analysis is the application of solid mechanics to predict the response (Interms of forces & displacements) of a given structure (existing or proposed) that subjected to a specified loads. LOADS (INPUTS) RESPONSE (INPUTS) STRUCTURE (SYSTEM)
  • 3. Loads are classified into 2 parts:  Dead loads (Self-weight; of the components of the structure).  Imposed loads & forces (Live, Wind, Snow, Rain, and Temperature, Erection loads, Seismic forces & others). The Structural Analysis is only ascertained correct when the following requirements were satisfied;-  Equilibrium Forces.  Compatibility of Displacement.  Force/Displacement Relations. Therefore, In every forms of the structures, the structural Engineer has to consider the following structural considerations and purposes.
  • 4.  Stability,  Strengths,  Stiffness,  Economy, as well as  Aesthetic aspects of the structure. The following Softwares are available  Orion,  STAAD III,  ANSYS,  AXIS VM,  ETABS, SAP, Etc
  • 5. #2 – DIFFERENT TYPES OF SUPPORTS  Roller,  Pinned,  Hinged,  Fixed,  Link,  Ball and Socket,  Rigid Support,  Spring Support. FORCES
  • 6. #2 – DIFFERENT TYPES OF STRUCTURES  Frame Structure,  Truss Structure,  Shell Structure,  Arch Structure,  Suspension Structure,  Mass Structure, &  Composite Structure.
  • 7.
  • 8. #3 – LIST OF EQUILIBRIUM EQUATIONS For state of static equilibrium to exist, it is necessary that the combined resultant effect of the system of forces shall be neither a Force nor a Couple; otherwise there will be tendency for motion of a body. However, many 3D structures are idealized as series of 2D components:  If the combined resultant effect of a general system of forces acting on a planar structures is not be equivalent to a resultant force, the algebraic sum of all F푥 components must be equal to Zero and the algebraic sum of all F푦 components must to be equal to Zero, i.e F푥 = 0 F푦 = 0.  If the combined resultant effect is not to be equivalent to a couple, the algebraic sum of the moment M푧 of all forces about any axis parallel to the Z-reference axis and normal to the plane of the structure must be equal to zero, i.e M푧 = 0 .
  • 9. #4 – DETERMINATE AND INDETERMINATE OF A STRUCTURE If the number of unknown forces is identical to the number of equilibrium equations, the problem is said to be Statically Determinate since the unknown forces can be determined directly from the equilibrium. 2푗 = 푚 + 푟 푤ℎ푒푟푒 푛 = 0 If, however the number of unknown forces exceeds the number of equilibrium equations, the problem is said to be Statically Indeterminate to a degree equal to this excess. 2푗 > 푚 + 푟 푤ℎ푒푟푒 푛 ≠ 0 푗 = 푁표. 표푓 푗표푖푛푡푠, 푚 = 푁표. 표푓 푚푒푚푏푒푟푠, 푟 = 푁표. 표푓 푟푒푎푐푡푖표푛푠
  • 10.
  • 11. #5 – TECHNIQUES USED IN ANALYSING STRUCTURE  Macaulay’s Method  Moment Area Method  Conjugate Beam Method  Virtual Work Method  Unit load Method  Influence line theory  The Three Moment Equation (Clapeyron’s Theorem)  Stiffness & Flexibility Method  Slope Deflection Method  Moment Distribution Method
  • 12. MACAULAY’S METHOD This is a method suggested by W. H. Macaulay to relate the stiffness, radius of curvature, deflection and the bending moments in a beam by integration methods. Beam Deflections using successive integration; Consider an infinitely small Section, dx, of the above loaded beam;
  • 13. MOMENT AREA METHOD  This is a method suitable for calculating slope & deflection at selected points on a beam.  It is also effective for calculating the deflections of beams with various cross sections.  The simplest way to evaluate the fixed -end moments, etc, will often be by the use of the Moment area method. There are two theorems associated with the moment area methods: First Moment Area Theorem: “The difference in slope between two points on a beam is equal to the area of the M/EI diagram between the two points.”
  • 14. Second Moment Area Theorem: “The moment about a point A of the M/EI diagram between points A and B will give the deflection of point A relative to the tangent at point B.” First Moment Area Theorem Second Moment Area Theorem
  • 15. #6 – INTRODUCTION TO FLEXIBILITY/STIFFNESS METHOD Flexibility Method (Force Method of Analysis) In this method, the degree of statical indeterminacy is initially determined. Thereafter, a number of releases equal to the degree of statical indeterminacy is introduced, each release being made by the removal of an external or internal force. Hence, the forces on the original indeterminate structure are calculated as the sum of the correction forces (redundants) and forces on the released structure. Flexibility Matrix [ f] ;- [f]{F} = {Δ − 퐷} D represents inconsistencies in deformation while {F} represents the redundants, Δ Elements represent prescribed displacements at their respective coordinates. The column vector {Δ - D} thus depends on the external loading.
  • 16. Stiffness Method (Displacement Method of Analysis) The displacement method can be applied to statically determinate or indeterminate structures, but is more useful in the latter, particularly when the degree of statical indeterminacy is high. In this method, one must first determine the degree of kinematic indeterminacy. A coordinate system is then established to identify the location and direction of joint displacements. Restraining forces equal in number to the degree of kinematic indeterminacy are introduced at the co-ordinates to prevent the displacement of the joints. Stiffness Matrix [S];- {D} = [푆]−1{-F} The elements of the vector {D} are the unknown displacements. The elements of the matrix [S] are forces corresponding to unit values of displacements. The column vector {F} depends on the loading on the structure.
  • 17. #3 – MATRIX OPERATIONS Let A, B, and C be mxn matrices. We have Properties involving Addition. 1. A+B = B+A 2. (A+B)+C = A + (B+C) 3. A+0 = A where is the mx zero-matrix (all its entries are equal to 0); 4. A+B = 0, if and only if B = -A.