Trusses - Method of Sections

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Trusses - Method of Sections ME 202 Methods of Truss Analsis Method of joints (previous notes) Method of sections (these notes) 2 MOS - Concepts Separate the structure into two parts (sections) b cutting through it. Draw an FBD of the section that is on one side or the other of the cut. Use method for non-concurrent, coplanar sstems. Yes-Yes The method of sections involves analzing non-concurrent, coplanar force sstems, and so uses moment summations. Three independent equations on the section. No more than three unknowns on a section. 3 4

MOS - Steps 1. Draw a FBD of the entire structure. 2. Solve for the structure s overall reactions. 3. Cut the truss to epose the force in a member of interest. Eample 1 Use method of sections to find forces in all members as functions of the applied load, F. A A 4. Draw a FBD of the section that is on one side or the other of the cut. 5. On the section s FBD, if possible, write an equilibrium equation in which the desired force is the onl unknown. C C 6. Repeat steps 3. - 5. as necessar. 5 C = C 6 M A = 0 C = 5 3 F A A C = C C = 5 3 F F = 0 A = C = 5 3 F C C A A M B = 0 F AC = 5 3 F F = 0 A = F C = 2 3 F C = C M A = 0 F BC = 5 3 F F = 0 F AB = 34 3 F A F AB F BC F AC F AB B 7

Eample 2 F BC Use the method of sections to find the force in member BE. F BE 3 kn F FE M D = 0 A = 3 kn A D F = 0 F BE = 0 D 9 10 Use the method of sections to find the force in member BF. Eample 3 Eample 4 F = 0 8 89 F BF 30 kip = 0 F BF F BF = 15 4 89 kip Use the method of sections to find the forces in members UV, MV, EM and DE. 11 12

13 14 M E F = 0 FEM = M V M D = 0 FUV = 15 15 P 4 16 = 0 FMV = = 0 FDE P 2 2 P 2 2 15 = P 4

Trusses - Method of Sections (MOS) 2 In previous notes, we have seen the method of joints (MOJ) for analzing trusses. In these notes, we will see the method of sections (MOS), which is ver different from the MOJ. There are several significant differences in these two methods. 3 If ou stud the eamples that follow, the meaning of the concepts on this slide should quickl become quite clear. 4 One difference between the MOJ and the MOS is that in the MOJ, we do not use moment summations, ecept perhaps in finding the overall reactions supporting the truss, while in the MOS, we use moment summations ver often. 5 For some simple problems, steps 1 and 2 can be skipped. One of the following eamples will have this propert. 1 of 5

6 A FBD of the entire structure includes reactions at A and C. Because of the rollers at C, the force there is normal to the inclined plane. Because we know the force s direction, we know the ratio of its rectangular components. So, the force there is onl one unknown. 7 The order of these summations is such that each contains onl one unknown. This completes steps 1 and 2. After finding the structure s overall reactions, we cut through members AB and BC and draw a FBD of the section to the right of the cut. Note that the moment summation is about a point that is not on the FBD. There is nothing incorrect about that. Given the force in member BC, the second summation has onl one unknown. 8 To find the force in member AC, we must make a cut that goes through member AC. Again, summing moments about a point that is not on the FBD gives an equation with onl one unknown. 9 Steps 1 and 2 are to find the overall reactions. But we can avoid finding the reactions at D if we cut the structure verticall between B and C and use a FBD of everthing to the left of the cut. That FBD will have three unknowns, which are the forces in members BC, EF and BE. 2 of 5

10 This problem illustrates a second difference between the MOJ and the MOS. In finding the force in a member in the interior of a truss, the MOJ requires that we analze first one joint and then another until we work our wa to a joint on which we can find the desired force. For a complicated truss this can require that we make man FBDs. But b using the MOS, we can often find the force in an interior member with onl one or two FBDs. 11 If we were to use the MOJ for this problem, we could start at joint D or joint E and work our wa to F or B, where we could find the required force. But with the MOS, we can find the force with onl one FBD and one equation. In this eample, finding the overall reactions is unnecessar. 12 The required forces are in the members highlighted in green. 13 A FBD of the entire structure can be used to find the reactions shown at point A on this slide. The FBD shown here results from cutting the structure verticall between joints U and V. Because the diagram has four unknowns, it is staticall indeterminate. 3 of 5

On a staticall indeterminate bod, we cannot find all the unknowns from the equations of statics. But we need them all for this problem. How man of the unknowns would we need to have to make this FBD staticall determinate? 14 The second cut eposes onl one of the desired unknown forces, which is the force in member UV. Of course, it also eposes forces in members MU, DL and CD, and so results in another FBD with four unknowns. While it ma seem that making the second cut does not get us an closer to a solution, the following slide demonstrates otherwise. 15 For three of the four unknowns, the line of action passes through point D. B summing moments about D, we have a single equation with the onl unknown being the force in member UV. Now, we can return to the first cut and have onl three unknowns. 16 Given the force in member UV, we can find each remaining unknown with a single equation. Note that the final equation has onl one unknown onl because it is written after the previous two equations. Note also that each triangle in the truss is an isosceles, right triangle. This means that the angle theta is 45, which simplifies computing the moments arms needed in the moment summations. 4 of 5

This problem illustrates a third difference between the MOJ and the MOS. Application of the MOJ requires little thought. B moving from joint to joint, analzing ever joint in the structure if necessar, we can eventuall find the force in ever member. With the MOS, we can usuall find the force in an specified member with onl one or two FBDs, but first we must see where to cut the structure to facilitate this. We also need to see what moment centers will ield equations with one unknown. The need to see which cuts and moment centers will lead us quickl to the desired result requires a higher level of thought than that needed for the MOJ. 5 of 5