FIGURE 17
^F 7 P 1 +P 2 + P 3 - 20,000 = O, or P 1 +P 2 + P 3 = 20,000, Eq. a; also, ^Mc = 16P 1 + 1OP 2
- 20,000(12) = O, or 16P 1 + 1OP 2 = 240,000, Eq. b.
- Establish the relations between the deformations
Selecting an arbitrary center of rotation O 9 show the bar in its deflected position (Fig.
lie). Establish the relationships among the three deformations. Thus, by similar triangles,
(AZ 1 - A/ 2 )/(A/ 2 - A/ 3 ) = 6/10, or 1OA/! - 16A/ 2 + 6A/ 3 = O, Eq. c. - Transform the deformation equation to an axial-force equation
By substituting axial-force relations in Eq. c, the following equation is obtained:
10Pi(5)/(1.25£) - 16P 2 (9)/(1.20E) + 6P 3 (I.S)IE = O, or 40Pi - 12OP 2 + 45P 3 = O, Eq. c'. - Solve the simultaneous equations developed
Solve the simultaneous equations a, b, and c' to obtain PI = 11,810 Ib (52,530 N); P 2 =
5100 Ib (22,684 N); P 3 = 3090 Ib (13,744 N).
5. Locate the center of rotation
To locate the center of rotation, compute the relative deformation of rods 1 and 2. Thus
A/! = 11,810(5)/(1.25£) = 47,240/£; A/ 2 = 5100(9)7(1.2OF) = 38,250/£.'
In Fig. 17c, by similar triangles, x/(x - 6) = A/!/A/ 2 = 1.235; x = 31.5 ft (9.6 m).
6. Verify the computed values of the tensile forces
Calculate the moment with respect to A of the applied and resisting forces. Thus MAa =
20,000(4) - 80,000 lb-ft (108,400 N-m); MAr = 5100(6) + 3090(16) = 80,000 lb-ft
(108,400 N-m). Since the moments are equal, the results are verified.
ANALYSIS OF CABLE SUPPORTING
A CONCENTRATED LOADA cold-drawn steel wire % in (6.35 mm) in diameter is stretched tightly between two
points lying on the same horizontal plane 80 ft (24.4 m) apart. The stress in the wire isDeflected position•Initial positionAssumed center
of rotation