03.06.2013 Views

5003 Lectures - Faculty of Engineering and Applied Science

5003 Lectures - Faculty of Engineering and Applied Science

5003 Lectures - Faculty of Engineering and Applied Science

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

E<strong>5003</strong> - Ship Structures I 59<br />

© C.G. Daley<br />

When we have bending moments in both y <strong>and</strong> z, there will be a line <strong>of</strong> zero axial<br />

stress that we call the heeled neutral axis. This is not necessarily aligned with the<br />

total moment. To find the heeled neutral axis we solve for the location <strong>of</strong> zero stress;<br />

σ<br />

X<br />

− M z cos θ M y sin θ<br />

w<br />

w<br />

= 0 =<br />

+<br />

,<br />

I NA<br />

I CL<br />

solving for z in terms <strong>of</strong> y , we get;<br />

I NA z = tan θ ⋅ y ,<br />

I CL<br />

I NA<br />

where we define: tan ψ = tan θ<br />

I CL<br />

z = tan ψ ⋅ y<br />

ψ is the angle <strong>of</strong> the heeled neutral axis from the y axis;

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!