fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
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FORCE<br />
A force is a vector quantity. It is defined when its (1)<br />
magnitude, (2) point <strong>of</strong> application, and (3) direction are<br />
known.<br />
RESULTANT (TWO DIMENSIONS)<br />
The resultant, F, <strong>of</strong> n forces with components Fx,i and Fy,i<br />
has the magnitude <strong>of</strong><br />
⎡⎛<br />
F = ⎢⎜<br />
∑<br />
⎢⎣<br />
⎝<br />
1<br />
2<br />
2 2<br />
1 1 ⎥ ⎥<br />
n ⎞ ⎛ n ⎞ ⎤<br />
Fx,<br />
i ⎟ + ⎜ ∑ Fy,<br />
i ⎟<br />
i=<br />
i=<br />
⎠<br />
⎝<br />
The resultant direction with respect to the x-axis using fourquadrant<br />
angle functions is<br />
θ =<br />
⎛ n<br />
arctan ⎜ ∑ F<br />
⎝ i=<br />
1<br />
y,<br />
i<br />
The vector form <strong>of</strong> a force is<br />
F = Fx i + Fy j<br />
n<br />
∑ F<br />
i=<br />
1<br />
⎠<br />
x,<br />
i<br />
RESOLUTION OF A FORCE<br />
Fx = F cos θx; Fy = F cos θy; Fz = F cos θz<br />
cos θx = Fx /F; cos θy = Fy /F; cos θz = Fz /F<br />
Separating a force into components (geometry <strong>of</strong> force is<br />
known R =<br />
2 2 2<br />
x + y + z )<br />
Fx = (x/R)F; Fy = (y/R)F; Fz = (z/R)F<br />
MOMENTS (COUPLES)<br />
A system <strong>of</strong> two forces that are equal in magnitude, opposite<br />
in direction, and parallel to each other is called a couple.<br />
A moment M is defined as the cross product <strong>of</strong> the radius<br />
vector r and the force F from a point to the line <strong>of</strong> action <strong>of</strong><br />
the force.<br />
M = r × F; Mx = yFz – zFy,<br />
My = zFx – xFz, and<br />
Mz = xFy – yFx.<br />
SYSTEMS OF FORCES<br />
F = Σ Fn<br />
M = Σ (rn × Fn)<br />
Equilibrium Requirements<br />
Σ Fn = 0<br />
Σ Mn = 0<br />
⎞<br />
⎟<br />
⎠<br />
⎦<br />
STATICS<br />
24<br />
CENTROIDS OF MASSES, AREAS, LENGTHS,<br />
AND VOLUMES<br />
Formulas for centroids, moments <strong>of</strong> inertia, and first<br />
moment <strong>of</strong> areas are presented in the MATHEMATICS<br />
section for continuous functions. The following discrete<br />
formulas are for defined regular masses, areas, lengths, and<br />
volumes:<br />
rc = Σ mnrn/Σ mn, where<br />
mn = the mass <strong>of</strong> each particle making up the system,<br />
rn = the radius vector to each particle from a selected<br />
<strong>reference</strong> point, and<br />
rc = the radius vector to the center <strong>of</strong> the total mass<br />
from the selected <strong>reference</strong> point.<br />
The moment <strong>of</strong> area (Ma) is defined as<br />
May = Σ xnan<br />
Max = Σ ynan<br />
Maz = Σ znan<br />
The centroid <strong>of</strong> area is defined as<br />
xac = May /A<br />
yac = Max /A<br />
zac = Maz /A<br />
where A = Σ an<br />
The centroid <strong>of</strong> a line is defined as<br />
xlc = (Σ xnln)/L, where L = Σ ln<br />
ylc = (Σ ynln)/L<br />
zlc = (Σ znln)/L<br />
The centroid <strong>of</strong> volume is defined as<br />
xvc = (Σ xnvn)/V, where V = Σ vn<br />
yvc = (Σ ynvn)/V<br />
zvc = (Σ znvn)/V<br />
MOMENT OF INERTIA<br />
The moment <strong>of</strong> inertia, or the second moment <strong>of</strong><br />
area, is defined as<br />
Iy = ∫ x 2 dA<br />
Ix = ∫ y 2 dA<br />
The polar moment <strong>of</strong> inertia J <strong>of</strong> an area about a point is<br />
equal to the sum <strong>of</strong> the moments <strong>of</strong> inertia <strong>of</strong> the area about<br />
any two perpendicular axes in the area and passing through<br />
the same point.<br />
Iz = J = Iy + Ix = ∫ (x 2 + y 2 ) dA<br />
= rp 2 A, where<br />
with respect to center <strong>of</strong><br />
the coordinate system<br />
rp = the radius <strong>of</strong> gyration (see page 25).