This document discusses the equilibrium of non-concurrent coplanar forces. It provides examples of solving for tensions, reactions, and angles in systems involving rods, cables, and other objects in equilibrium under various loading conditions. Solutions are shown using free body diagrams and summing moments and forces. Key steps include reducing the system to a resultant force and couple, setting the linear and rotational components equal to zero, and solving the resulting equations for the unknown values.
This powerpoint presentation deals mainly about bearing stress, its concept and its applications.
Members:
BARIENTOS, Lei Anne
MARTIREZ, Wilbur
MORIONES, Jan Ebenezer
NERI, Laiza Paulene
Sir Romeo Alastre - MEC32/A1
This is a lecture on normal stress in mechanics of deformable bodies. There is a quick overview on what strength of materials is at the beginning of the presentation.
Presentation by:
MEC32/A1 Group 1 4Q 2014
MAGBOJOS, Redentor V.
RIGOR, Lady Krista V.
SALIDO, Lisette S.
Mapúa Institute of Technology
Presentation for Prof. Romeo D. Alastre's class.
This powerpoint presentation deals mainly about bearing stress, its concept and its applications.
Members:
BARIENTOS, Lei Anne
MARTIREZ, Wilbur
MORIONES, Jan Ebenezer
NERI, Laiza Paulene
Sir Romeo Alastre - MEC32/A1
This is a lecture on normal stress in mechanics of deformable bodies. There is a quick overview on what strength of materials is at the beginning of the presentation.
Presentation by:
MEC32/A1 Group 1 4Q 2014
MAGBOJOS, Redentor V.
RIGOR, Lady Krista V.
SALIDO, Lisette S.
Mapúa Institute of Technology
Presentation for Prof. Romeo D. Alastre's class.
This is first or introductory lecture of Mechanics of Solids-1 as per curriculum formulated by Higher Education Commission and Pakistan Engineering Council
This is first or introductory lecture of Mechanics of Solids-1 as per curriculum formulated by Higher Education Commission and Pakistan Engineering Council
Lec.2 statically determinate structures & statically indeterminate struct...Muthanna Abbu
The student will learn the determination of internal forces in different structures and the
kind of forces distribution due to external & internal effects .He will also learn about the
structures deformation due to these effects .
In Engineering Mechanics the static problems are classified as two types: Concurrent and Non-Concurrent force systems. The presentation discloses a methodology to solve the problems of Concurrent and Non-Concurrent force systems.
Engmech 06 (equilibrium of non_concurrent force system)
1. EQUILIBRIUM OF NON-CONCURRENT COPLANAR FORCES
The figure shows a general coplanar force system. It was shown in our previous discussion that such
general coplanar force system may be reduced to a resultant force R and/or a resultant couple M acting in
the same plane.
For the body to be in equilibrium, both linear displacement due to R, and the rotation due to couple M
should be zero.
Example:
A boom AC hinged at A supports a 400 N load as shown. Find the force in cable BC, which is attached to
the wall at B. Neglect self weight of boom. And also solve for the reactions at hinge A.
Solution:
From our previous example, we solved this problem knowing that the forces are concurrent at
point C and we found out that the tension in the cable is T = 292.82 N.
This time, we will consider the FBD of the boom AC to solve for the tension in the wire T, as well
as the reaction of the wall at hinge A. Notice that the forces at the boom are non-current.
FBD:
2. ∑ MA = 0
(Consider CCW rotation Positive)
(T sin 75 o )(2 m) − (400N sin 45 o )(2m) = 0
T = 292.82 N
To solve for the reactions at the hinge A; we will take the summation of forces at the horizontal
and vertical directions.
[∑ F x = 0] → +
R AH − (292.82N) cos 30 o = 0
RAH = 253.59 N
[∑ Fy ]
=0 ↑+
R AV + (292.82N) sin 30 o − 400 = 0
RAV = 253.59 N
Assignment:
(1) An 8 kg slender rod AB is attached to two collars which may slide along guides without friction shown.
Determine for equilibrium of rod AB (a) Angle θ (b) the reactions at A and B.
Ans. 49.11o, RA = 45.31 N, RB = 90.62 N
(2) A slender rod of length “L” and weight “W” is held in equilibrium position as shown. Determine the angle θ
and tension in each cable.
Ans. TAB = 0.596W, θ = 59.21o, TCD = 1.164W
3. (3) A 3m bar AB of negligible weight is to be kept in horizontal position as shown; Neglecting friction,
determine distance ‘x’ if P = 300N. Also find the value of ‘P’ if x = 1.5m.
(4) A 200 N cylinder is supported on an 80 N member AB. Find ‘W’ to be attached to the rope neglecting
friction mass and size of pulley. Take diameter of cylinder 750 mm and length of member AB to be 3m.
What will be components of reaction at end A?
Ans. W=117.65N, HA= 98.1N, VA= 221.18N
(5) A 150 N weight is held in equilibrium by a 5 kg uniform bar AB hinged at A as shown. Determine (a)
components of reactions at A and (b) tension in cable DC. Take length of bar 1m.
Ans. T = 604.6 N, HA = 302.3 N, VA = 324.5 N