Vector Mechanics for Engineers: Statics
Vector Mechanics for Engineers: Statics
12th Edition
ISBN: 9781259977268
Author: Ferdinand P. Beer, E. Russell Johnston Jr., David Mazurek
Publisher: McGraw-Hill Education
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Chapter 6.2, Problem 6.56P

A Pratt roof truss is loaded as shown. Determine the force members FH, FI, and GI.

Chapter 6.2, Problem 6.56P, A Pratt roof truss is loaded as shown. Determine the force members FH, FI, and GI. Fig. P6.55 and

Fig. P6.55 and P6.56

Expert Solution & Answer
Check Mark
To determine

The force in the members FH,FIand GI.

Answer to Problem 6.56P

The force in the members FH,FIand GI are, 10.0 kN which is a compressive force, 4.92kN and 6.00kN both of which are tension forces respectively.

Explanation of Solution

The Pratt roof truss is loaded as shown in the figure. There is load at all the point on the top. The free body diagram of the given arrangement is given by Figure 1.

 Vector Mechanics for Engineers: Statics, Chapter 6.2, Problem 6.56P , additional homework tip  1

Figure 1

The total load on the truss is given from the figure as,

Total load=5(3kN)+2(1.5kN)=18kN

By symmetry the y component of the reaction at A will be half the total load.

Ay=12(18kN)=9kN

The section’s free body diagram is given as,

Vector Mechanics for Engineers: Statics, Chapter 6.2, Problem 6.56P , additional homework tip  2

The tangent of the angle α can be written from the diagram as,

tanα=6.753

The angle is derived from the tangent value as,

α=tan16.753=66.04°

From the diagram the sum of the moments in the counter clockwise direction about I is given as,

45FFH(23×6.75m)+Ay(6m)(1.5kN)(6m)(3kN)(3m)=0 (I)

From the diagram the sum of the moments in the counter clockwise direction about L is given as,

FFI(sinα)(6m)(3kN)(6m)(3kN)(3m)=0 (II)

From the diagram the sum of the moments in the counter clockwise direction about H is given as,

FGI(6.75m)+(1.5kN)(9m)+(3kN)(3m)+(3kN)(6m)Ay(9m)=0 (III)

Conclusion:

Solve for FFH from (I) by substituting 9kN for Ay.

{45FFH(23×6.75m)+(9kN)(6m)(1.5kN)(6m)(3kN)(3m)}=0FFH={(9kN)(6m)+(1.5kN)(6m)+(3kN)(3m)}45(23×6.75m)=10.0 kN

Solve for FDE from (II) by substituting 66.04° for α.

{FFI(sin(66.04°))(6m)(3kN)(6m)(3kN)(3m)}=0FFI=(3kN)(6m)+(3kN)(3m)(sin(66.04°))(6m)=+4.92kN

Solve for FDF from (III) by substituting 9kN for Ay.

{FGI(6.75m)+(1.5kN)(9m)+(3kN)(3m)+(3kN)(6m)(9kN)(9m)}=0FGI={(1.5kN)(9m)(3kN)(3m)(3kN)(6m)+(9kN)(9m)}(6.75m)=+6.00kN

Therefore, the force in the members FH,FIand GI are, 10.0 kN which is a compressive force, 4.92kN and 6.00kN both of which are tension forces respectively.

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Chapter 6 Solutions

Vector Mechanics for Engineers: Statics

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