(Part A) Machinerys Handbook 31st Edition Pages 1-1484

Machinery's Handbook, 31st Edition

170 Force Systems Finding the Resultant of Nonparallel Forces Not Meeting at a Common Point:

z

The diagram shows a system of noncoplanar, nonparallel, noncon­ current forces F 1 , F 2 , etc. for which the resultant is to be determined. Generally speaking, the resultant will be a noncoplanar force and a couple, which may be further com­ bined, if desired, into two forces that are skewed. This is the most general force system that can be devised, so each of the other systems so far described represents a special, simpler case of this general force system. The method of solution described below for a system of three forces applies for any number of forces.

F 2

F 1

O

y

x 2 z 2

y 2

F 3

x

1) Select a set of coordinate x , y , and z axes at any desired point O in the body as shown in the diagram. 2) Determine the x , y , and z coordinates of any convenient point on the line of action of each force as shown for F 2 . Also determine the angles, θ x , θ y , θ z that each force makes with each coordinate axis. These angles are measured counterclockwise from the positive direction of the x , y , and z axes. The data is tabulated, as shown in the table accompanying Step 3, for convenient use in subsequent calculations. 3) Calculate the x , y , and z components of each force using the formulas given in the accompanying table. Add these components algebraically to get ∑ F x , ∑ F y and ∑ F z , which are the components of the resultant R given by the formula, R F F F x y z 2 2 2 R R R = + + ^ ^ ^ h h h

Force

Coordinates of Force F

Components of F

F x y

z

F x

F y

F z

θ x

θ y

θ z

F 1 cos θ x 1 F 2 cos θ x 2 F 3 cos θ x 3

F 1 cos θ y 1 F 2 cos θ y 2 F 3 cos θ y 3

F 1 cos θ z 1 F 2 cos θ z 2 F 3 cos θ z 3

F 1 F 2 F 3

x 1 x 2 x 3

y 1 y 2 y 3

z 1 z 2 z 3

θ x 1

θ y 1

θ z 1

θ x 2

θ y 2

θ z 2

θ x 3

θ y 3

θ z 3

∑ F x

∑ F y

∑ F z

The resultant force R makes angles of θ xR , θ yR , and θ zR with the x , y , and z axes, respectively, and passes through the selected point O . These angles are determined from the formulas,

cos cos cos

F R F R F R x y z ' ' '

= = =

i i i

R R R

xR yR zR

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