Fork E Join

and maintenance while still providing platform flexibility. Consider the following guidelines when designing for portability: l Make full use of the native RIA code libraries and design for the goal of “write once, run everywhere,” but be willing to fork code in cases where overall project complexity or feature tradeoffs dictate that you must do so. l When deciding whether to design a RIA or a Web application, consider that the differences between browsers will require Web applications…

EVALUATE: 2 x − x0 = 2 2 vx − v0 x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

EVALUATE: 2 x − x0 = 2 2 vx − v0 x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

EVALUATE: 2 x − x0 = 2 2 vx − v0 x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

EVALUATE: vx2 − v02x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 2 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

EVALUATE: 2 x − x0 = 2 2 vx − v0 x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

EVALUATE: 2 x − x0 = 2 2 vx − v0 x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

EVALUATE: 2 x − x0 = 2 2 vx − v0 x v2 = − 0 x . If his initial speed had been 45 mi/h he would have stopped in 2a x 2ax 5.81. ⎛ 45 mi/h ⎞ ⎜ ⎟ (192 ft) = 91 ft . ⎝ 65.5 mi/h ⎠ ! ! IDENTIFY: Apply ∑ F = ma to the point where the three wires join and also to one of the balls. By symmetry the tension in each of the 35.0 cm wires is the same. 5-36 Chapter 5 The geometry of the situation is sketched in Figure 5.81a. The angle φ that each wire makes with the 12.5 cm and φ…

solved it that evening after dinner. He published the solution anonymously, but on seeing it, Johann Bernoulli exclaimed, “Ah, I know the lion by his paw.” Daniel Bernoulli (1700–1782), son of Johann, migrated to St. Petersburg as a young man to join the newly established St. Petersburg Academy, but returned to Basel in 1733 as professor of botany, and later, of physics. His interests were primarily in partial differential equations and their applications. For instance, it is his…