Skip to main content

Analysis of Bars due to Axial loads

Determination of stress, strain and deformations in the bars subjected to axial loads.

Principle of Superposition

The resultant deformation of the body is equal to the algebraic sum of the deformation of the individual section. Such principle is called as principle of superposition
In the analysis of axial loaded bars we use the principle of superposition. By draw the free body diagrams of each section of the bar for finding out the required stresses and strains or deformations. we can understand the concept with the following example.
Example:
Q.1. Determine the stress in each section of the bar shown in the figure.The PQ and RS segments are having a length of 1 meter and QR segment is 1.5 m.  The cross section of bar is 10 mm square. What will be the total extension of the bar? The Young's modulus of bar material E = 210000 MPa.
Solution :
Check the equilibrium of the bar, the sum of total forces in X- axis is ∑ Fx = 0
                          - 63 + 35 + 49 - 21 = 0
Write the free body diagram of the each portion of the bar

The each part of the bar should be in equilibrium by introducing the internal forces as shown in the above fig.

1.Segment- PQ
The area of the bar = A = 10x10 =100 mm2
The axial tensile force acting in left side of segment  P1 = + 63 kN
For equilibrium the right side of the segment is also subjected to same force P1 = + 63 kN
The stress in segment PQ =
s1 = P1/A = 63000/100 =63N/mm2 (Tensile stress)
The elongation in segment PQ =ΔL1 =PL/AE
ΔL1 = (63000x1000)/ (100x2100000) = 0.3 mm
Segment-2, QR
The area of the bar = A = 10x10 =100 mm2
The axial tensile force in segment QR =
The right side net internal force P2 =
     (+P1) - 35 = 63 - 35 = + 28kN 
The axial tensile stress in segment 2 =
s2 = P2/A = 28000/100 = 280N/mm2
The elongation in segment QR =ΔL2 =PL/AE
ΔL2 = (28000x1500)/ (100x2100000) = 0.2 mm
3.Segment- RS
The area of the bar = A = 10x10 =100 mm2
The axial compressive force acting left side of  segment RS =
 P3 = - 21kN =-21000 N
Check: The internal force on right side of the segment is = p2 - 49 = 28 - 49 = -21kN
The stress in segment 3 =
s3 =  P3/A = - 21000/100 
               = -210 N/mm2 (compressive stress)
The shortening in segment 3 =ΔL3= PL/AE
ΔL3 = (-21000x1000)/ (100x2100000) = -0.1 mm
The total extension of the bar is equal to sum of the extensions of all three segments PQ,QR,RS
ΔL= ΔL1+ ΔL2+ΔL3
ΔL = 0.3 + 0.2 - 0.1 = 0.4 mm 

The Deformations of bars of varying sections

Let us see the following figure, where we can see a bar of having different length and different cross-sectional area and bar is subjected with an axial load P. 
As we can see here that length and cross-sectional areas of each section of bar is different and therefore stress induced, strain and change in length too will be different for each section of bar.
Young’s modulus of elasticity of each section might be same or different depending on the material of the each section of bar.



Axial load for each section will be same i.e. P. When we will go to determine the total change in length of the bar of varying sections, we will have to add change in length of each section of bar.
P = Bar is subjected here with an axial Load
A1, A2 and A3 = Area of cross section of section 1, section 2 and section 3 respectively
L1, L2 and L3 = Length of section 1, section 2 and section 3 respectively
σ1, σ2 and σ3 = Stress induced for the section 1, section 2 and section 3 respectively
ε1, ε2 and ε3 = Strain developed for the section 1, section 2 and section 3 respectively
E = Young’s Modulus of the bar
Let us see here stress and strain produced for the section 1
Stress, σ1= P / A1
Strain, ε1 = σ1/E = (P/AE)1
Similarly stress and strain produced in the section 2
Stress, σ2= P / A2
Strain, ε2 = σ2/E =
(P/AE)2
Similarly stress and strain produced for the section 3
Stress, σ3= P / A3
Strain, ε3 = σ3/E = (P/AE)3
Now we will determine change in length for each section with the help of definition of strain
ΔL= (PL/AE)1
ΔL(PL/AE)2
ΔL3  (PL/AE)3
Total change in length of the bar
To determine the total change in length of the bar of varying sections, we will have to add change in length of each section of the bar.
ΔL= ΔL1+ ΔL2+ΔL3


Assignment :
1.A copper bar shown in figure is subjected to a tensile load of 30 KN. Determine elongation of the bar if E=100 GPa. Also find maximum stress induced.

2.
A bar of uniform cross sectional area 100mm2 is subjected to forces as shown below. Calculate the change in the length of the bar.Young's modulus of material is 200 GPa

Comments

Popular posts from this blog

Relation between Modulus of Elasticity and Modulus of Rigidity

Modulus of Elasticity (E)   It is the ratio between Normal stress to Normal strain within the elastic limit. Elastic Modulus E = Normal stress/Normal strain E =  s/e Modulus of Rigidity (G)  It is the ratio between Shear stress to Shear strain within the elastic limit. Rigidity Modulus G = Shear stress/ Shear strain G =    Ƭ / ø   Relation between Modulus of Elasticity and Modulus of Rigidity: Consider a solid cube  PQRS is  subjected to a shearing force F.  Let  Ƭ     be the shear stress produced in the faces PQ and RS due to this shear force. The complementary shear stress consequently produced in the vertical faces PS and RQ is also equal to same and shown in figure as Ƭ   Due to the pure shearing force, the cube is deformed PQRS to PQR'S' . The point   S moved to S' and point R moved to R' as shown in fig.  The shear strain = The angle of distortion  ø           ...

Shearing Stresses Distribution in Circular Section

Show that the shearing stress developed at the neutral axis of a beam with circular cross section is  τ max = (4/3)(F/πr2). Assume that the shearing stress is uniformly distributed across the neutral axis.  Solution : Let us consider the circular section of a beam as displayed in following figure. We have assumed one layer EF at a distance y1 from the neutral axis of the circular section of the beam Shear stress at a section will be given by following formula as mentioned here Where, F = Shear force (N) τ = Shear stress (N/mm2) A = Area of section, where shear stress is to be determined (mm2) ȳ = Distance of C.G of the area, where shear stress is to be determined, from neutral axis of the beam section (m) Q = A. ȳ = Moment of the whole shaded area about the neutral axis I = Moment of inertia of the given section about the neutral axis (mm4) For circular cross-section, Moment of inertia, I = ПR4/4 b = Width of the given section where shear stress is to be determined. Let us co...

PORTAL METHOD and CANTILEVER METHOD

The behavior of a structure subjected to horizontal forces depends on its height to width ratio. The deformation in low-rise structures, where the height is smaller than its width, is characterized predominantly by shear deformations. In high rise building, where height is several times greater than its lateral dimensions, is dominated by bending action. To analyze the structures subjected to horizontal loading we have two methods. Portal method  and Cantilever method 1. PORTAL METHOD The portal method is an approximate analysis used for analysing building frames subjected to lateral loads such as Wind loads/ seismic forces.  Since shear deformations are dominant in low rise structures, the method makes simplifying assumptions regarding horizontal shear in columns.  Each bay of a structure is treated as a portal frame, and horizontal force is distributed equally among them. Assumptions in portal method   1. The points of inflection are located at the mid-height of e...