Determine the lengths of cords ACB and CO. The knot at C is located midway between A and B.
A blog where I post solutions to the mechanics and statics problems that I encounter. Also many mastering engineering problems will be seen, so users of that program may find this blog interesting. The course uses the Hibbeler Statics textbook and some of the subjects covered include: Cartesian vectors, force resultants, force equilibrium, particle equilibrium, Hooke's Law, vector decomposition, etc. More to be added as those problems and topics are encountered.
Showing posts with label Stretch. Show all posts
Showing posts with label Stretch. Show all posts
Tuesday, October 6, 2015
Wednesday, September 16, 2015
3_1_h
Determine the mass of each of the two cylinders if they cause a sag of s = 0.5 m when suspended from the rings at A and B. Note that s = 0 when the cylinders are removed.
3_1_g
A continuous cable of total length 4 m is wrapped around the small pulleys at A, B, C, and D. If each spring is stretched 300 mm, determine the mass m of each block. Neglect the weight of the pulleys and cords. The springs are unstretched when d = 2 m.
3_1_e
The unstretched length of spring AB is 2 m. If the block is held in the equilibrium position shown, determine the mass of the block at D.
Labels:
2D Equilibrium,
Components,
Force,
Force Equilibrium,
Force Vectors,
Hooke's Law,
Particles,
Spring,
Springs,
Statics,
Stretch,
sum,
Vector
Wednesday, February 18, 2015
3: Notes
Particle Equilibrium
It is necessary to draw a free body diagram to account for all the forces that act on a particle
FR = ΣF = 0
2D
ΣFx = 0
ΣFy = 0
TENSION & pulleys - The tension force in a continuous cable that passes over a pulley is constant throughout the cable to keep it in equilibriumΣFy = 0
SPRING - If the problem involves an elastic spring, then the stretch or compression (s) of the spring can be related to the force applied to it
F = ks
3D
ΣFNET = 0
ΣFx = 0
ΣFy = 0
ΣFz = 0
ΣFx = 0
ΣFy = 0
ΣFz = 0
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