Section Modulus calculation and optimization
Report On Section Modulus Calculation Of Hood
INTRODUCTION
To calculate the section modulus of the previously designed hood for analyzing its strength and also optimizing the design to see the difference in the bending strength of the hood. Higher the section modulus of a structure, the more the resistive it becomes to bending.
Section modulus
Section modulus is a geometric property for a given cross-section used in the design of beams or flexural members, it is also referred to as the Polar Modulus or the Torsional Sectional Modulus. Other geometric properties used in design include area for tension and shear, radius of gyration for compression, and moment of inertia and polar moment of inertia for stiffness. Any relationship between these properties is highly dependent on the shape in question. Equations for the section moduli of common shapes are given below. There are two types of section moduli, the elastic section modulus and the plastic section modulus.
S=I/Y
Here,
S = Section modulus
I= Moment of Inertia (Unit mm 4)
Y= Distance from Neutral axis to the extreme end (unit mm)
The Unit of a “section modulus” is (mm3)
Elastic section modulus
For general design, the elastic section modulus is used, applying up to the yield point for most metals and other common materials.
The elastic section modulus is defined as S = I / y, where I is the second moment of area (or area moment of inertia, not to be confused with moment of inertia) and y is the distance from the neutral axis to any given fibre. It is often reported using y = c, where c is the distance from the neutral axis to the most extreme fibre, as seen in the table below. It is also often used to determine the yield moment (My) such that My = S × σy, where σy is the yield strength of the material.
Plastic section modulus
The plastic section modulus is used for materials where elastic yielding is acceptable and plastic behavior is assumed to be an acceptable limit. Designs generally strive to ultimately remain below the plastic limit to avoid permanent deformations, often comparing the plastic capacity against amplified forces or stresses.
The plastic section modulus depends on the location of the plastic neutral axis (PNA). The PNA is defined as the axis that splits the cross section such that the compression force from the area in compression equals the tension force from the area in tension. So, for sections with constant yielding stress, the area above and below the PNA will be equal, but for composite sections, this is not necessarily the case.
The plastic section modulus is the sum of the areas of the cross section on each side of the PNA (which may or may not be equal) multiplied by the distance from the local centroids of the two areas to the PNA:

the Plastic Section Modulus can also be called the 'First moment of area'
The plastic section modulus is used to calculate the plastic moment, Mp, or full capacity of a cross-section. The two terms are related by the yield strength of the material in question, Fy, by Mp=Fy*Z. Plastic section modulus and elastic section modulus are related by a shape factor which can be denoted by 'k', used for an indication of capacity beyond elastic limit of material. This could be shown mathematically with the formula :-

shape factor for a rectangular section is 1.5.
So here we are Calculating Elastic section Modulus
| Cross-sectional shape | Figure | Equation | Comment |
|---|---|---|---|
| Rectangle | ![]() |
Solid arrow represents neutral axis | |
| doubly symmetric I-section (major axis) |
|
NA indicates neutral axis | |
| doubly symmetric I-section (minor axis) | ![]() |
NA indicates neutral axis | |
| Circle | ![]() |
Solid arrow represents neutral axis | |
| Circular hollow section | ![]() |
Solid arrow represents neutral axis | |
| Rectangular hollow section | ![]() |
NA indicates neutral axis | |
| Diamond | ![]() |
NA indicates neutral axis | |
| C-channel | ![]() |
NA indicates neutral axis |
First Design Study
The Intersection of the design was taken and then section Inertia Analysis was done-


Moment of inertia(max) = 7.557011989e×10^5×mm^4
Moment of inertia(min) = 2.694133773e×10^3×mm^4
Y=485.7599/2=242.8799 mm
S=I/Y
S=2.69413×10^3/242.87= 11.09288 mm^3
Hood Design Optimization
By increasing the depth of the inner panel by 0.5 mm


Moment of inertia(max) = 7.557011989e×10^5×mm^4
Moment of inertia(min) = 2.694133773e×10^3×mm^4
Y=485.7599/2=242.8799 mm
S=I/Y
S=7.5570×10^3/242.87=31.11541 mm^3
So the strength of an hood varies from11.09288 mm^3 to 31.11541 mm^3
- So, here when comparing both the hoods there is changes in both MAX and MIN strength values,what i came to know that when i increased sectional area by 1mm the value of minimum strength was increased from 11.09288 mm^3 to31.11541 mm^3 ,Hence with increase in cross sectional area results in increase in strength.
- But, when we seen the value of maximum strength its slightly decreases from 11.09288 mm^3to31.11541 mm^3
,i think this due to design of hood, here what we want to know that when increase in cross sectional area there will be increase in minimum strength or maximum strength or increase in both. - So Newton's first law also explains that ,if higher the mass , the force required to move the object is also high due to offering more resistance in order to move the object, This resistance we called it as a MOMENT OF INERTIA.
- In case of hood also same principle will work, i.e when increase in cross sectional area by 1mm the minimum load carrying capacity or strength was increased by approximately 8% percentage what we observed from the above discussion.
- The strength of the material also depends upon the composition of material ,thickness and cross sectional area of an object.
CONCLUSION
The strength of the material is directly proportional to the moment of inertia, hence increase in sectional area there is have increase in overall mass of an object ,hence have increase in strength.

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