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Exam (elaborations)

Solution Manual for Engineering Statics: Friction - Chapter 8 (Beer and Johnston Style)

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This exhaustive solution manual provides detailed, step-by-step mathematical and graphical analysis for problems in Chapter 8, focusing on the laws of dry friction and their applications in mechanical systems. Drawing from comprehensive sources, this document covers the fundamental techniques required to solve complex engineering problems involving wedges, square-threaded screws, journal bearings, thrust bearings, and belt friction. You will find high-level guidance on determining whether a system will slip or tip, as well as calculating the forces required for motion. Key highlights of this resource include: • Dry Friction Analysis: Solutions for packages on conveyor belts and crates on inclined planes, including determining coefficients of static (μ s ​ ) and kinetic (μ k ​ ) friction. • Wedges and Screws: Detailed analysis of wedge-driven splitting, gear-pulling assemblies, and square-threaded screws used in jacks and high-strength bolts. • Bearings and Axles: Mastery of friction circles for journal bearings and the calculation of torque in thrust bearings and axles for vehicles like scooters. • Belt Friction & Pulleys: Comprehensive coverage of flat belts and V-belts, including the derivation and application of the tension formula (T 2 ​ =T 1 ​ e μβ ) for flywheels, pulleys, and band brakes. • Advanced Mechanical Devices: Analysis of self-locking strap wrenches, eccentric cams for safety devices, and pipe-gripping Stillson wrenches. • Mathematical Rigor: Problems are solved using equilibrium equations (ΣF=0,ΣM=0) and force triangles across both SI and US Customary units (N, kN, lb, kips). This manual is an indispensable tool for engineering students looking to master structural analysis and the behavior of members under the influence of friction.

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CHAPTER 8
V

, PROBLEMV8.1

DetermineVwhetherVtheVblockVshownVisVinVequilibriumVandVfindVtheVma
gnitudeVandVdirectionVofVtheVfrictionVforceVwhenP=V150VN.




SOLUTION

AssumeVequilibrium
:




FxV =V0:V V FV +V(500V N)VsinV 20V−V(150V N)Vc
osV 20V=V0
FV =V −30.056V NV FV =V30.056V N

F =V0:V V NV −V(500VN)VcosV20V−V(150VN)Vsi
NV =V +521.15V NV NV =V521.
15V N

MaximumVfrictionVforc
e:
FmV =VsVN
=V0.30(521.15V
N)
= 156.345 N
SinceVFVis blockVisVinVequilibrium
andV FV VF ◀
FV =V30.1VN
20.0




CopyrightV©VMcGraw-
HillVEducation.VPermissionVrequiredVforVreproductionVorVdisplay.

, PROBLEMV8.2

DetermineVwhetherVtheVblockVshownVisVinVequilibriumVandVfindVtheVma
gnitudeVandVdirectionVofVtheVfrictionVforceVwhenVP=V400VN.




SOLUTION

AssumeVequilibrium
:




FxV =V0:V V FV +V(500V N)VsinV 20°V−V(400V N)VcosV 20°V=
V0

FV =V +204.87V N
FV =V 204.87
VN

F = 0: N − (500 N) cos 20 − (400 N) sin 20 =

MaximumVfrictionVforc FmV =VsVN
e: =V0.30(606.65V
N)
=V181.995VN
Since FV  V blockVmovesVup
F , ◀
ActualVfrictionVforc FV =V FkV =V kVNV =V0.25(606.6 FV =V151.7V N
e: 5V N) 20.0




CopyrightV©VMcGraw-
HillVEducation.VPermissionVrequiredVforVreproductionVorVdisplay.

, PROBLEMV8.3

DetermineV whetherV theV blockV shownV isV inV equilibriumV andV fi
ndV theVmagnitudeVandVdirectionVofVtheVfrictionVforceVwhenVPV=
V120Vlb.




SOLUTION

AssumeVequilibrium
:




FxV =V0:V V FV +V(50V lb)VsinV 30V−V(120V lb)VcosV40V=
V0

FV =V +66.925V
lb

FyV =V0:V V NV −V(50Vlb)VcosV30V−V(120Vlb)VsinV40V=V0
MaximumVfrictionVforce:
FmV =VsVN
=V0.40(120.436Vl
b)
=V48.174Vlb
blockVmovesVup
WeVnoteVthatV FVVFmV.V Thus, ◀
VActualVfrictionVforce:
FV =V36.1 30.0V
FV = V F =V VNV =V0.30(120.436V lb)V=V36.131Vlb, Vlb ◀




CopyrightV©VMcGraw-
HillVEducation.VPermissionVrequiredVforVreproductionVorVdisplay.

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