28.12.2013 Views

Chapter 2 Review of Forces and Moments - Brown University

Chapter 2 Review of Forces and Moments - Brown University

Chapter 2 Review of Forces and Moments - Brown University

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

2.2.2 Resultant moment exerted by a force system.<br />

(1) (2) ( N )<br />

(1) (2) ( N )<br />

Suppose that N forces F , F ... F act at positions r , r ,... r . The resultant moment <strong>of</strong> the<br />

force system is simply the sum <strong>of</strong> the moments exerted by the forces. You can calculate the resultant<br />

moment by first calculating the moment <strong>of</strong> each force, <strong>and</strong> then adding all the moments together (using<br />

vector sums).<br />

Just one word <strong>of</strong> caution is in order here – when you compute the resultant moment, you must take<br />

moments about the same point for every force.<br />

Taking moments about a different point for each force <strong>and</strong> adding the result is meaningless!<br />

2.2.3 Examples <strong>of</strong> moment calculations using the vector formulas<br />

We work through a few examples <strong>of</strong> moment calculations<br />

Example 1: The beam shown below is uniform <strong>and</strong> has weight<br />

W. Calculate the moment exerted by the gravitational force about<br />

points A <strong>and</strong> B.<br />

We know (from the table provided earlier) that the center <strong>of</strong><br />

W<br />

gravity is half-way along the beam.<br />

The force (as a vector) is<br />

F = −Wj<br />

To calculate the moment about A, we take the origin at A. The position vector <strong>of</strong> the force relative to A is<br />

r = ( L /2) i<br />

The moment about A therefore<br />

MA = r× F= ( L/ 2) i× ( − W) j =−( WL/ 2) k<br />

To calculate the moment about B, we take B as the origin. The position vector <strong>of</strong> the force relative to B is<br />

r = −( L /2) i<br />

Therefore<br />

MB = r× F= ( − L/ 2) i× ( − W) j = ( WL/ 2) k<br />

Example 2. Member AB <strong>of</strong> a ro<strong>of</strong>-truss is subjected to a vertical gravitational force W <strong>and</strong> a horizontal<br />

wind load P. Calculate the moment <strong>of</strong> the resultant<br />

B<br />

force about B.<br />

P j<br />

Both the wind load <strong>and</strong> weight act at the center <strong>of</strong><br />

W<br />

i<br />

gravity. Geometry shows that the position vector <strong>of</strong><br />

θ<br />

the CG with respect to B is<br />

A<br />

r = ( −L/ 2) i−( L/ 2) tanθ<br />

j<br />

2L<br />

The resultant force is<br />

F= Pi−Wj<br />

Therefore the moment about B is<br />

A<br />

j<br />

L<br />

B<br />

i

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

Saved successfully!

Ooh no, something went wrong!