With the force P appliced on a member, the stress distributions at different cross sections are different as shown below. However, at locations far enough away from the support and the applied load, the stress distribution becomes uniform. This is due to: a b C (a) O Inelastic property Poisson's effect -C Saint Venant's Principle O Principle of superposition section a-a section b-b (b) section - section e-c av ²

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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  1. With the force P appliced on a member, the stress distributions at different cross sections are different as shown below. However, at locations far enough away from the support and the applied load, the stress distribution becomes uniform. This is due to:



                 
     

       

    Inelastic property

       

    Poisson’s effect

       

    Saint Venant’s Principle

       

    Principle of superposition

With the force P appliced on a member, the stress distributions at different cross sections are different as shown below. However, at locations far enough
away from the support and the applied load, the stress distribution becomes uniform. This is due to:
a
b
C
(a)
O Inelastic property
Poisson's effect
-C
Saint Venant's Principle
O Principle of superposition
section a-a
section b-b
(b)
section -
section e-c
av
²
Transcribed Image Text:With the force P appliced on a member, the stress distributions at different cross sections are different as shown below. However, at locations far enough away from the support and the applied load, the stress distribution becomes uniform. This is due to: a b C (a) O Inelastic property Poisson's effect -C Saint Venant's Principle O Principle of superposition section a-a section b-b (b) section - section e-c av ²
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