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and doubling, we have for semi-circle,

0

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If we divide G by the area of the semi-circle, we obtain the distance from the centre of the circle to the centre of gravity of the semi-circle,

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Elliptic Section.-The Ellipse is immediately derived from the circle thus:-Let the ellipse, fig. 117, have the same minor diameter as the circle above it, so that b2r; all the vertical dimensions of the circle are, however, to be altered in the constant ratio a: r, since the vertical radius of the circle is altered to a. Let the circle be divided into rectangular elements, each with an edge lying on the neutral axis; when the circle is changed into the ellipse, each element remains of the same breadth bas before, but its vertical dimension is changed from y to Y, where Y: y::a:r.

K

r

Y:y::a:r

k----

Fig.117.

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For each element, and therefore for the whole figure, the moment of inertia

has changed in the ratio

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For a semi-ellipse about a diameter as axis, we have

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Hollow Circular Section.-For a hollow circle or ellipse the reduction is the same as for the hollow rectangle, page 237,

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136. Find the moment of resistance to bending of the symmetrical section, the upper half of which is shown in fig. 118; the material is wrought iron, for which the weaker working strength is fa= 4 tons per square inch.

Consider the two triangles as one of breadth 8 inches; for a triangle about its own neutral axis, I = bh3 = 48; hence for semi-section

江。

= (48+24 × 82) for triangle+ × 2(103-03) forrectangle.

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137. For the cross section shown in fig. 119, and which is the semi-section shown in fig. 118, find the working value of M, if the working strengths of the material be f = 4, and fo 5 tons per square inch.

=

Choose BB as an axis of reference; then

S=24+20=44; G2 = (24 × 8) + 1⁄2 × 2(102 −02) = 292. II of example 136, = 2251.

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138. Find M for the section, the upper half of which is shown in fig. 120; the material is cast iron, for which f 2 tons per square inch.

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For the cross section,

11 = (201+50·26 × 82) + } × 3(43 — 03).

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fo

-I = 126964 1161 inch-tons.

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139. Find M for the section shown in fig. 121, the working strengths fa and f, being 4 and 5 tons per square inch respectively.

It is convenient to choose CC the diameter of the ellipse as the axis of reference, and we have

Ellipse.
S=π × 4 × 3+

Middle rect.
3 x 6

+

Lower rect.
10 x 2

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π

= 75·7; 0 + 1 × 3(92 − 32) + 1⁄2 × 10(112 — 92) = 308;

Ic= × 8 × 63 + 1 × 3(93 − 33) + 1⁄2 × 10(113— 93) = 2793;

64

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= 4 inches sensibly; so that y. = 7, and

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= 7 inches.

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The neutral axis being sensibly in the middle, take ƒ = 4 the smaller strength, and M = 1,

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904 inch-tons.

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140. Find the resistance to bending for the section shown in fig. 122; the dimensions are in inches, and the strengths

R

=

of the material are fa 4 tons (thrust), and f = 5 tons (tension) per square inch.

Choose CC the diameter of the ellipse as an axis of reference; and for semi-ellipse

S= 236; Go-30; I, 53.

=

For semi-circle about its diameter, I 245, and distance. from centre to g its centre of gravity is 2:12 inches; hence about its own neutral axis, that is an axis through g, we have I ̧ = I – S(2·12)2 = 69; and for semi-circle—

S = 393; G = 398; I = 4093.

For the two triangles, reckoned as one about its own neutral axis I= 427; hence for double triangle

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y= 8.3 ins., and y. = 77 ins.; and I ̧ =

5

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= '602;

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Уз

8.3

taking the smaller value, we have

M5191 1167 inch-tons.

As shown in the figure, the section is lying in a position suitable for a cantilever; if intended for a beam, it should be turned upside down; should it be kept as it stands, however, then for a beam we take the smaller of the two viz., 482; multiplying I, by this

ratios,

5 7.7

and

4 8.3'

quantity gives a value of M, which is less than the above.

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