Further Reduction of a Force and Couple System
(Section 4.9)
If FR and MRO are perpendicular to each other, then the system can be further reduced to a single force, FR , by simply moving FR from O to P.
In three special cases, concurrent, coplanar, and parallel systems of forces, the system can always be reduced to a single force.
Example #1
Given: A 2D force and couple system as shown.
Find: The equivalent resultant force and couple moment acting at A and then the equivalent single force location along the beam AB.
Plan:
Example #1
+ → Σ FRx = 25 + 35 sin 30° = 42.5 lb
+ ↓ Σ FRy = 20 + 35 cos 30° = 50.31 lb
+ MRA = 35 cos30° (2) + 20(6) – 25(3) = 105.6 lb∙ft
FR = ( 42.52 + 50.312 )1/2 = 65.9 lb
θ = tan-1 ( 50.31/42.5) = 49.8 °
The equivalent single force FR can be located on the beam AB at a distance d measured from A.
d = MRA/FRy = 105.6/50.31 = 2.10 ft.
Example #2
Given: The building slab has four columns. F1 and F2 = 0.
Find: The equivalent resultant force and couple moment at the origin O. Also find the location (x,y) of the single equivalent resultant force.
Plan:
Example #2
FRO = {50 k – 20 k} = {70 k} kN
MRO = (10 i) × (20 k) + (4 i + 3 j)x(50 k)
= {200 j + 200 j – 150 i} kN∙m
= {150 i + 400 j } kN∙m
The location of the single equivalent resultant force is given as,
x = MRyo/FRzo = 400/(70) = 5.71 m
y = MRxo/FRzo = (150)/(70) = 2.14 m
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1. What is the concept of reduction of a force and couple system? |
2. How can the reduction of a force and couple system be applied in real-life scenarios? |
3. What are the steps involved in reducing a force and couple system? |
4. How does the reduction of a force and couple system simplify calculations and analysis? |
5. Can the reduction of a force and couple system be applied to three-dimensional systems? |
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