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Engineering Mechanics: Statics, SI Units (15th Edition, 2023, eBook) by Hibbeler

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The 15th Edition (SI Units) of Engineering Mechanics: Statics by R.C. Hibbeler delivers a student-focused, visual approach to learning core statics concepts. This fully digital eBook includes updated problem sets, clear illustrations, and real-world engineering applications using SI units. Topics include vector mechanics, particle and rigid body equilibrium, distributed forces, trusses, frames, internal forces, centroids, and friction. Designed for mechanical, civil, structural, and aerospace engineering students, the eBook format enables interactive learning on any device — perfect for exam prep, homework, and in-class study. engineering mechanics statics, statics si units, hibbeler statics 15th edition, engineering statics ebook, r.c. hibbeler statics, statics 2022 edition, si units statics textbook, statics digital textbook, mechanical engineering statics, civil engineering statics, statics for engineers, statics force analysis, vector mechanics statics, structural mechanics ebook, hibbeler statics online, statics course material, statics free body diagrams, trusses and frames statics

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Uploaded on
September 10, 2025
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Written in
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E-TEXTBOOK

, GLOBAL
EDITION


Engineering Mechanics
STATICS
Fifteenth Edition in SI Units




R. C. Hibbeler




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@seismicisolation

,SI Prefixes

Multiple Exponential Form Prefix SI Symbol
1 000 000 000 109 giga G
6
1 000 000 10 mega M
3
1 000 10 kilo k

Submultiple
0.001 10-3 milli m
0.000 001 10 -6
micro μ
0.000 000 001 10 -9
nano n




Conversion Factors (SI) to (FPS)

Unit of Unit of
Quantity Measurement (SI) Equals Measurement (FPS)
Force N 0.2248 lb
Mass kg 0.06852 slug
Length m 3.281 ft




@seismicisolation
@seismicisolation

,Fundamental Equations of Statics

Cartesian Vector Equilibrium
A = Axi + Ayj + Azk
Particle
Magnitude
A = 2A2x + A2y + A2z
ΣFx = 0, ΣFy = 0, ΣFz = 0
Rigid Body-Two Dimensions
Directions
ΣFx = 0, ΣFy = 0, ΣMO = 0
A Ax Ay Az
uA = = i + j + k Rigid Body-Three Dimensions
A A A A
= cos ai + cos bj + cos gk ΣFx = 0, ΣFy = 0, ΣFz = 0
cos2 a + cos2 b + cos2 g = 1 ΣMx = 0, ΣMy = 0, ΣMz = 0
Dot Product
A · B = AB cos u Friction
= AxBx + AyBy + AzBz Static (maximum) Fs = μsN
Cross Product Kinetic F k = μkN

3 Az 3
i j k
C = A : B = Ax Ay Center of Gravity
Bx By Bz Particles or Discrete Parts
Cartesian Position Vector Σ∼r W
r =
r = (x2 - x1)i + (y2 - y1)j + (z2 - z1)k ΣW
Body
Cartesian Force Vector

L

F = Fu = Fa b
r r dW
r r =

L
Moment of a Force dW

MO = Fd
Area and Mass Moments of Inertia
= r : F = 3 rx rz 3
i j k


L L
MO ry
I = r 2dA I = r 2dm
Fx Fy Fz

Moment of a Force about a Specified Axis Parallel-Axis Theorem
I = I + Ad 2 I = I + md 2
M = u # r : F = 3 rx rz 3
ux uy uz
ry Radius of Gyration
Fx Fy Fz
AA Am
I I
k = k =
Simplification of a Force and Couple System
FR = ΣF Virtual Work
( MR ) O = ΣM + ΣMO dU = 0

@seismicisolation
@seismicisolation

,Geometric Properties of Line and Area Elements
Centroid Location Centroid Location Area Moment of Inertia
y y
L 5 2ur A 5 ur 2
r r
u u 1 4 1
x x Ix = r (u - sin 2u)
C C 4 2
u u
r sin u 2 r sin u 1 4 1
u Iy = r (u + sin 2u)
3 u 4 2
Circular arc segment Circular sector area

y y9 1 4
Ix = πr
16
A 5 14 pr 2 1 4
L 5 p–2 r L 5 pr 4r Iy = πr
— 16
r 3p
x9
r C
Ix′ = a - b r4
2r
— C r x π 4
C p
4r

16 9 π
3p
Iy′ = a - b r4
π 4
Quarter and semicircle arcs Quarter circle area 16 9 π

a A 5 –12 h (a 1 b) y
pr 2
A5—
2 1 4
C Ix = πr
h x 4r 8

3p
r
–1 2 a 1 b h C
b 3 a 1b x 1 4
Iy = πr
8
Trapezoidal area Semicircular area

y
b A5 23– ab A 5 pr2
1
r Ix = πr4
a C 3– 4
5a x
C
1
3–
Iy = πr4
8b
4

Semiparabolic area Circular area


1 y A 5 bh
A5 —
3
ab 1 3
b Ix = bh
C 3
— b h x 12
10 C
–3 a
4 1 3
a b Iy = hb
12
Exparabolic area Rectangular area
a y9
1
A 5— bh
b 2
1 3
C h Ix′ = bh
h C x9 36

3
4 ab 1
A 5— b
3 —
3 Iy′ = hb3
b 36
2

5
a
Parabolic area Triangular area
@seismicisolation
@seismicisolation

,Center of Gravity and Mass Moment of Inertia of Homogeneous Solids
z z


r
V 5 pr 2 h
V5 4–3 pr 3 r h

G G 2

y h
– y
2
x
x
Cylinder
Sphere
1 1
2 Ixx = Iyy = m(3r2 + h2) Izz = mr2
Ixx = Iyy = Izz = mr2 12 2
5
z
z

1
V 5 – r 2h h
3 –
G 4 h
V 5 –23 pr 3
G y
r y r
x
x 3
–r Cone
8
3 3
Hemisphere Ixx = Iyy = m(4r2 + h2) Izz = mr2
80 10
2 z
Ixx = Iyy = 0.259 mr2 Izz = mr2
5

z
z9

G
G y
r a
b
y
x
x Thin plate
Thin circular disk 1 1 1
Ixx = mb2 Iyy = ma2 Izz = m(a2 + b2)
1 1 3 12 12 12
Ixx = Iyy = mr2 Izz = mr2 Iz′z′ = mr2
4 2 2 z

z
l
2
G
r y
x l
G 2
y
y9
x x9

Thin ring Slender rod
1 1 1
Ixx = Iyy = mr2 Izz = mr2 Ixx = Iyy = ml 2 Ix′x′ = Iy′y′ = ml 2 Iz′z′ = 0
2 12 3
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@seismicisolation
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,ENGINEERING MECHANICS




STATICS
FIFTEENTH EDITION IN SI UNITS




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