CIVL 3121 Virtual for Trusses 1/4

Principle of Virtual Work Principle of Virtual Work

 The principle of virtual work was developed by John  In 1738, Johann and his son Daniel nearly simultaneously Bernoulli in 1717 and is sometimes referred to as the published separate works on hydrodynamics. unit-load method.  Daniel is said to have had a bad relationship with his father  Johann Bernoulli (1667–1748; also known as Jean or John) was a Swiss mathematician  Upon both of them entering and tying and was one of the many prominent for first place in a scientific contest at mathematicians in the Bernoulli family. the University of Paris, Johann, unable to bear the "shame" of being  He is known for his contributions to infinitesimal compared Daniel's equal, banned calculus and educated in his youth. Daniel from his house.

Principle of Virtual Work Principle of Virtual Work

 In 1738, Johann and his son Daniel nearly simultaneously published separate works on hydrodynamics.  Daniel is said to have had a bad relationship with his father  Johann Bernoulli also plagiarized some key ideas from Daniel's book Hydrodynamica in his own book Hydraulica which he backdated to before Hydrodynamica.  Despite Daniel's attempts at reconciliation, his father carried the grudge until his death.

Truss – Virtual Work Truss – Virtual Work

 Virtual work is a procedure for computing a single  The system created by the actual loads is called component of deflection at any point on a structure. the P-system.

 To compute a component of deflection by the method of  As the structure deforms under the actual loads, external virtual work WQ is done by the virtual loads as they move virtual work, the designer applies a force to structure at the through real displacements. point and in the direction of the desired .  Due to the conversation of an equivalent quantity of  The force is called the dummy load or the virtual load. virtual strain energy UQ is stored in the structure.  The force system created by the virtual loads is called W = U the Q-system. Q Q CIVL 3121 Virtual Work for Trusses 2/4

Truss – Virtual Work Truss – Virtual Work

Consider the method of virtual work applied to one-bar truss, Now consider the and displacements produced by the as shown below. virtual load, as shown below.

WP - real work UP - real strain done by P energy stored in WD - real work UD - real strain AB due to P done by Q energy stored in AB due to Q WP = UP WD = UD

Truss – Virtual Work Truss – Virtual Work

Now consider the forces and displacements produced by the By the principle of , it follows virtual load and actual loads acting together. that WQ = UQ.

WT = UT

WT – total work UT - total strain WQ = UQ done by Q and P energy due to Q WQ = QP and P

Truss – Virtual Work Truss – Virtual Work

By the principle of conservation of energy, it follows By the principle of conservation of energy, it follows

that WQ = UQ. that WQ = UQ.

UQ = FQLP QP = FQLP CIVL 3121 Virtual Work for Trusses 3/4

Truss – Virtual Work Truss – Virtual Work

 By summing the energy expression for each member in a  Typically, the virtual load Q is assumed to be 1 and truss, we get: dimensionless.

QFLPQP   Therefore, the virtual work expression for the a single displacement component in the direction of the applied  The bar elongation LP can be compute is terms of the actual load P and the properties of the section. virtual load Q is: FL nNL F P nNL QFLPQP  Q    AE  P    AE AE Where n is the force in each member of the truss due to the virtual load and N is the force in each member of the truss due to the real loads.

Truss – Virtual Work Example 1 Truss – Virtual Work Example 1

Example: Compute the horizontal displacement at joint B in the truss Example: Compute the horizontal displacement at joint B shown below. Assume the E = 30,000 kip/in2, the area of bars AD and BC = 5 in2; the area of all other bars = 4 in2. . The value and direction of each real force is indicated on the truss.

. A (+) sign is tension and (–) sign is compression.

Real Force System

Truss – Virtual Work Example 1 Truss – Virtual Work Example 1

Example: Compute the horizontal displacement at joint B

. The value and direction of each virtual force is indicated on the truss.

2 2 . A (+) sign is tension and Member N (kips) nL(in) A (in ) NnL/A (kip in/in ) (–) sign is compression. AB 80 1 240 4 4,800

BC 100 0 300 5 0

CD -80 0 240 4 0

AD -100 -1.25 300 5 7,500 Virtual Force System BD -60 0 180 4 0

12,300 (kip/in) CIVL 3121 Virtual Work for Trusses 4/4

Truss – Virtual Work Example 1 Truss – Virtual Work Example 2

Therefore the horizontal displacement a joint B may Example: Compute the magnitude and direction of the displacement at joint D in the truss shown below. Assume the E = 29,000 kip/in2 and that the area of be computed as: each bars is given in parenthesis (in2).

12,300kip / in Forces due to real loads Bx  2 0.41in D 30,000kip / in D

3 ft (1.5) 15.09 C Member N (kips) nL(in) A (in2) NnL/A (kip in/in2) C 18 k 18 k AB 80 1 240 4 4,800 (1.5) -11.25

BC 100 0 300 5 0 (2.5) (3.0) 8 ft 22.5 -28.19 CD -80 0 240 4 0

AD -100 -1.25 300 5 7,500 A (1.5) B A -13.5 B BD -60 0 180 4 0

12,300 (kip/in) 6 ft 6 ft

Truss – Virtual Work Example 2 Truss – Virtual Work Example 2

Example: Compute the magnitude and direction of the displacement at joint Example: Compute the magnitude and direction of the displacement at joint D in the truss shown below. Assume the E = 29,000 kip/in2 and that the area of D in the truss shown below. Assume the E = 29,000 kip/in2 and that the area of each bars is given in parenthesis (in2). each bars is given in parenthesis (in2).

2 Forces due to vertical virtual loads Forces due to horizontal virtual loads Member N (kips) nV nH L (in) A (in ) NnVL/A (kip/in) NnHL/A (kip/in) D D AB -13.5 -0.75 -0.37 72 1.5 486.0 239.76 0.84 1.52 1 AC 22.5 1.25 2.29 120 2.5 1,350.0 2,473.20 C C 1 BC -11.25 -0.63 -1.15 96 1.5 453.6 828.0

-0.63 -1.15 BD -28.19 -1.57 -0.77 150.35 3.0 2,218.08 1,087.92 1.25 -1.57 2.29 -0.77 CD 15.09 0.84 1.52 84.49 1.5 713.97 1,231.2

5,188.2 (kip/in) 5,860.08 (kip/in) A B A -0.75 -0.37 B

Truss – Virtual Work Example 2 End of Virtual Work - Trusses

Therefore the total displacement a joint D may be computed as: Any questions? 5,860.08kip / in   0.20 in DH 29,000kip / in2 5,188.2kip / in D  2 0.18 in V 29,000kip / in

D 0.20 in 22 D 0.18in 0.20 in 0.27in   42

1 0.18in  0.18 in   tan  42 0.27 in 0.20in