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Building Design and Construction Handbook - Merritt - Ventech!

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STRUCTURAL THEORY 5.29<br />

Circular Sections. If a circular shaft (hollow or solid) is twisted, a section that is<br />

plane before twisting remains plane after twisting. Within the proportional limit,<br />

the shearing unit stress at any point in a transverse section varies with the distance<br />

from the center of the section. The maximum shear, psi, occurs at the circumference<br />

<strong>and</strong> is given by<br />

where T � torsional moment, in-lb<br />

r � radius of section, in<br />

J � polar moment of inertia, in 4<br />

Tr<br />

v � (5.43)<br />

J<br />

Polar moment of inertia of a cross section is defined by<br />

2 J � � � dA (5.44)<br />

where � � radius from shear center to any point in the section<br />

dA � differential area at the point<br />

In general, J equals the sum of the moments of inertia above any two perpendicular<br />

axes through the shear center. For a solid circular section, J � �r 4 /2. For a hollow<br />

circular section with diameters D <strong>and</strong> d, J � �(D 4 � d 4 )/32.<br />

Within the proportional limits, the angular twist between two points L inches<br />

apart along the axis of a circular bar is, in radians (1 rad � 57.3�):<br />

TL<br />

� � (5.45)<br />

GJ<br />

where G is the shearing modulus of elasticity (see Art. 5.2.4).<br />

Noncircular Sections. If a shaft is not circular, a plane transverse section before<br />

twisting does not remain plane after twisting. The resulting warping increases the<br />

shearing stresses in some parts of the section <strong>and</strong> decreases them in others, compared<br />

wit the sharing stresses that would occur if the section remained plane. Consequently,<br />

shearing stresses in a noncircular section are not proportional to distances<br />

from the share center. In elliptical <strong>and</strong> rectangular sections, for example, maximum<br />

shear occurs on the circumference at a point nearest the shear center.<br />

For a solid rectangular section, this maximum may be expressed in the following<br />

form:<br />

T<br />

v � (5.46)<br />

2 kb d<br />

where b � short side of rectangle, in<br />

d � long side, in<br />

k � constant depending on ratio of these sides;<br />

d/b � 1.0 1.5 2.0 3 4 5 10 �<br />

k � 0.208 0.231 0.246 0.258 0.267 0.282 0.291 0.312 0.333<br />

(S. Timoshenko <strong>and</strong> J. N. Goodier, ‘‘Theory of Elasticity,’’ McGraw-Hill Publishing<br />

Company, New York.)

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