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Shawn Kenny, Ph.D., P.Eng. Assistant Professor Faculty of Engineering and Applied Science Memorial University of Newfoundland ENGI.

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Presentation on theme: "Shawn Kenny, Ph.D., P.Eng. Assistant Professor Faculty of Engineering and Applied Science Memorial University of Newfoundland ENGI."— Presentation transcript:

1 Shawn Kenny, Ph.D., P.Eng. Assistant Professor Faculty of Engineering and Applied Science Memorial University of Newfoundland spkenny@engr.mun.ca ENGI 1313 Mechanics I Lecture 22:Equivalent Force Systems and Distributed Loading

2 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 2 Lecture 22 Objective to demonstrate by example equivalent force systems to determine an equivalent force for a distributed load

3 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 3 Example 22-01 Handle forces F 1 and F 2 are applied to the drill. Replace this system by an equivalent resultant force and couple moment acting at point O. Express the results in Cartesian vector form.

4 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 4 Equivalent Distributed Loads Reduce to Single Equivalent Load  Magnitude and position Applications  Environment Wind Fluid  Dead load Weight Snow, sand Objects

5 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 5 Distributed Loads Load Intensity  Pressure (Pa) Force per unit area N/m 2 or lb/ft 2  Infinite # parallel vertical loads Reduce from Area to Line Load

6 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 6 Distributed Loads (cont.) Consider Element Length (dx)  Element force (dF) acts on element length (dx)  The line load w(x) represents force per unit length

7 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 7 Distributed Loads (cont.) Magnitude Net Force (F R )  Summation of all element forces  Area under line load curve

8 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 8 Distributed Loads (cont.) Resultant Moment (M Ro )  Element force moment  Total moment  Equivalent force

9 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 9 Distributed Loads (cont.) Centroid  Geometric center of area  Resultant force line of action

10 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 10 Example 22-02 Determine equivalent resultant force and location for the following distributed load. L/2

11 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 11 Example 22-03 Determine equivalent resultant force and location for the following distributed load. L/3

12 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 12 Comprehension Quiz 22-01 What is the location of F R or distance d?  A) 2 m  B) 3 m  C) 4 m  D) 5 m  E) 6 m Answer: D FRFR 3 m d

13 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 13 Example 22-04 The beam is subjected to the distributed loading. Determine the length b of the uniform load and its position a on the beam such that the resultant force and couple moment acting on the beam are zero.

14 ENGI 1313 Statics I – Lecture 22© 2007 S. Kenny, Ph.D., P.Eng. 14 References Hibbeler (2007) http://wps.prenhall.com/esm_hibbeler_eng mech_1


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