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The process of reducing distributed loads to a single equivalent force in engineering analysis. Students will learn about uniform distributed loads, the magnitudes and locations of resultant forces, and the concept of centroids. examples of rectangular and triangular loading diagrams and provides formulas for finding the resultant force and its location. In-class activities include quizzes, group problem solving, and attention quizzes.
Typology: Lecture notes
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In-Class Activities:
Today’s Objectives:
Students will be able to determine an equivalent force for a distributed load.
(continued)
The uniform wind pressure is acting on a triangular sign (shown in light brown).
To be able to design the joint between the sign and the sign post, we need to determine a single equivalent resultant force and its location.
In such cases, w is a function of x and has units of force per length.
In many situations, a surface area of a body is subjected to a distributed load. Such forces are caused by winds, fluids, or the weight of items on the body’s surface. We will analyze the most common case of a distributed pressure loading. This is a uniform load along one axis of a flat rectangular body.
The total moment about point O is given as
Assuming that FR acts at 𝑥𝑥 ̅, it will produce the moment about point O as
The force dF will produce a moment of (x)(dF) about point O.
LOCATION OF THE RESULTANT FORCE (continued)
Comparing the last two equations, we get
You will learn more detail later, but FR acts through a point “C,” which is called the geometric center or centroid of the area under the loading curve w(x).
The rectangular load: FR = 400 × 10 = 4,000 lb and x= 5 ft. The triangular loading: FR = (0.5) (600) (6) = 1,800 N and = 6 – (1/3) 6 = 4 m. Please note that the centroid of a right triangle is at a distance one third the width of the triangle as measured from its base.
x
Now let’s complete the calculations to find the concentrated loads (which is a common name for the resultant of the distributed load).
C) Area D) Volume
x
w
FR
y Distributed load curve
Given : The loading on the beam as shown. Find : The equivalent force and its location from point A. Plan:
For the left triangular loading of height 800 lb/ft and width 12 ft, F (^) R1 = (0.5)(800) x 12 = 4800 lb
𝑥𝑥 � 1 =(2/3)(12) = 8ft from A
For the rectangular loading of height 500 lb/ft and width 9ft,
F (^) R3 = (500)(9) = 4500 lb
and its line of action is as 𝑥𝑥� 3 =(1/2)(9) + 12 = 16.5ft from A
For the top right loading of height 300 lb/ft and width 9 ft,
F (^) R2 = (0.5)(300)(9) = 1350 lb
and its line of action is at 𝑥𝑥� 2 =(1/3)(9) + 12 = 15ft from A
GROUP PROBLEM SOLVING (continued)
GROUP PROBLEM SOLVING (continued)
4800 lb (^) 4500 lb
1350 lb
8 ft
16.5 ft
15 ft
For the combined loading of the three forces, add them.
F (^) R = 4800 + 4500 +1350 = 10650 lb
Now, (F (^) R 𝑥𝑥�) has to equal MRA = 132.9 kip-ft
So solve for 𝑥𝑥� to find the equivalent forces locations.
Hence, 𝑥𝑥� = (132.9 kip-ft) / (10.65 kip) = 12.5 ft from A