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"BEAMANAL" --- SINGLE-SPAN and CONTINUOUS-SPAN BEAM ANALYSIS
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Program Description:
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"BEAMANAL" is a spreadsheet program written in MS-Excel for the purpose of analysis of either single-span or
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continuous-span beams subjected to virtually any type of loading configuration. Four (4) types of single-span beams
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and two (2) through (5) span, continuous-span beams, considered. Specifically, beam end reactions as well as the
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maximum moments and deflections are calculated. Plots of both the shear and moment diagrams are produced,
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as well as a tabulation of the shear, moment, slope, and deflection for the beam or each individual span. Also, for
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steel single-span beams an AISC 9th Edition (ASD) Code check can be performed for X-axis bending and shear.
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This program is a workbook consisting of four (4) worksheets, described as follows:
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Worksheet NameDescription
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DocThis documentation sheet
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Single-Span BeamSingle-span beam analysis for simple, propped, fixed, & cantilever beams
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Single-Span Beam & Code CheckSingle-span beam analysis and AISC Code Check for X-axis bending
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Continuous-Span BeamContinuous-span beam analysis for 2 through 5 span beams
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Program Assumptions and Limitations:
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1. The following reference was used in the development of this program (see below):
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"Modern Formulas for Statics and Dynamics, A Stress-and-Strain Approach"
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by Walter D. Pilkey and Pin Yu Chang, McGraw-Hill Book Company (1978), pages 11 to 21.
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2. This program uses the three (3) following assumptions as a basis for analysis:
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a. Beams must be of constant cross section (E and I are constant for entire span length).
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b. Deflections must not significantly alter the geometry of the problem.
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c. Stress must remain within the "elastic" region.
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3. On the beam or each individual span, this program will handle a full length uniform load and up to eight (8) partial
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uniform, triangular, or trapezoidal loads, up to fifteen (15) point loads, and up to four (4) applied moments.
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4. For single-span beams, this program always assumes a particular orientation for two (2) of the the four (4)
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different types. Specifically, the fixed end of either a "propped" or "cantilever" beam is always assumed to be on
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the right end of the beam.
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5. This program will calculate the beam end vertical reactions and moment reactions (if applicable),
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the maximum positive moment and negative moment (if applicable), and the maximum negative deflection
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and positive deflection (if applicable). The calculated values for the end reactions and maximum moments
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and deflections are determined from dividing the beam into fifty (50) equal segments with fifty-one (51) points,
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and including all of the point load and applied moment locations as well. (Note: the actual point of maximum
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moment occurs where the shear = 0, or passes through zero, while the actual point of maximum deflection is
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where the slope = 0.)
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6. The user is given the ability to input two (2) specific locations from the left end of the beam to calculate the
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shear, moment, slope, and deflection.
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7. The user is also given the ability to select an AISC W, S, C, MC, or HSS (rectangular tube) shape to aide in
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obtaining the X-axis moment of inertia for input for the purely analysis worksheets.
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8. The plots of the shear and moment diagrams as well as the displayed tabulation of shear, moment, slope,
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and deflection are based on the beam (or each individual span) being divided up into fifty (50) equal segments
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with fifty-one (51) points.
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9. For continuous-span beam of from two (2) through five (5) spans, this program utilizes the "Three-Moment
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Equation Theory" and solves a system simultaneous equations to determine the support moments
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10. This program contains numerous “comment boxes” which contain a wide variety of information including
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explanations of input or output items, equations used, data tables, etc. (Note: presence of a “comment box”
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is denoted by a “red triangle” in the upper right-hand corner of a cell. Merely move the mouse pointer to the
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desired cell to view the contents of that particular "comment box".)
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Formulas Used to Determine Shear, Moment, Slope, and Deflection in Single-Span Beams
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For Uniform or Distributed Loads:
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Loading functions for each uniform or distributed load evaluated at distance x = L from left end of beam:
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FvL =
-wb*(L-b-(L-e)) + -1/2*(we-wb)/(e-b)*((L-b)^2-(L-e)^2)+(we-wb)*(L-e)
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FmL =
-wb/2*((L-b)^2-(L-e)^2) + -1/6*(we-wb)/(e-b)*((L-b)^3-(L-e)^3)+(we-wb)/2*(L-e)^2
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FqL =
-wb/(6*E*I)*((L-b)^3-(L-e)^3) + -1/(24*E*I)*(we-wb)/(e-b)*((L-b)^4-(L-e)^4)+(we-wb)/(6*E*I)*(L-e)^3
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FDL =
-wb/(24*E*I)*((L-b)^4-(L-e)^4) + -1/(120*E*I)*(we-wb)/(e-b)*((L-b)^5-(L-e)^5)+(we-wb)/(24*E*I)*(L-e)^4
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Loading functions for each uniform or distributed load evaluated at distance = x from left end of beam:
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If x >= e:
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Fvx =
-wb*(x-b-(x-e)) + -1/2*(we-wb)/(e-b)*((x-b)^2-(x-e)^2)+(we-wb)*(x-e)
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Fmx =
-wb/2*((x-b)^2-(x-e)^2) + -1/6*(we-wb)/(e-b)*((x-b)^3-(x-e)^3)+(we-wb)/2*(x-e)^2
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Fqx =
-wb/(6*E*I)*((x-b)^3-(x-e)^3) + -1/(24*E*I)*(we-wb)/(e-b)*((x-b)^4-(x-e)^4)+(we-wb)/(6*E*I)*(x-e)^3
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FDx =
-wb/(24*E*I)*((x-b)^4-(x-e)^4) + -1/(120*E*I)*(we-wb)/(e-b)*((x-b)^5-(x-e)^5)+(we-wb)/(24*E*I)*(x-e)^4
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else if x >= b:
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Fvx =
-wb*(x-b) + -1/2*(we-wb)/(e-b)*(x-b)^2
else:Fvx =0
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Fmx =
-wb/2*(x-b)^2 + -1/6*(we-wb)/(e-b)*(x-b)^3-(x-e)^3
else:Fmx =0
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Fqx =
-wb/(6*E*I)*(x-b)^3 + -1/(24*E*I)*(we-wb)/(e-b)*(x-b)^4
else:Fqx =0
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FDx =
-wb/(24*E*I)*(x-b)^4 + -1/(120*E*I)*(we-wb)/(e-b)*(x-b)^5
else:FDx =0
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For Point Loads:
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Loading functions for each point load evaluated at distance x = L from left end of beam:
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FvL =-P
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FmL =-P*(L-a)
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FqL =
-P*(L-a)^2/(2*E*I)
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FDL =
P*(L-a)^3/(6*E*I)
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Loading functions for each point load evaluated at distance = x from left end of beam:
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If x > a:
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Fvx =-Pelse:Fvx =0
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Fmx =-P*(x-a)else:Fmx =0
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Fqx =
-P*(x-a)^2/(2*E*I)
else:Fqx =0
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FDx =
P*(x-a)^3/(6*E*I)
else:FDx =0
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For Applied Moments:
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Loading functions for each applied moment evaluated at distance x = L from left end of beam:
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FvL =0
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FmL =-M
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FqL =-M*(L-c)/(E*I)
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FDL =
M*(L-c)^2/(2*E*I)
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Loading functions for each applied moment evaluated at distance = x from left end of beam: