A problem about virtual work principle

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SUMMARY

The discussion focuses on applying the virtual work principle to derive equilibrium equations for a continuous mechanical system, specifically a long thin bar fixed at one end and subjected to pressure P at the other end. The user struggles to derive the correct equilibrium equations, particularly emphasizing the importance of considering the neglected third term in their calculations. The user notes that the terms from their equation result in T δu |_0^L = 0, which does not provide a condition on T due to δu(0) = δu(L) = 0. Expert advice is sought to clarify this issue.

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athosanian
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hello, I want to apply the virtual work principle to a continuous mechanical system to derive equilibrium equation, naemly, a long thin bar with one end fixed in the wall and other end applied with pressure P. but I can not derive the correct equilibrium equations. I hope some expert could give some advice.
my thhinking is shown below:
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?temp_hash=1576381b83a3354a61cab8b6a348bfb3.png


?temp_hash=1576381b83a3354a61cab8b6a348bfb3.png
 

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Obviously, if the two terms from (4) result in ## T \delta u |_0^L = 0 ##, which gives you no condition on ##T## because ## \delta u(0) = \delta u(L) = 0 ##, it is the neglected third term that you must take into account.
 

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