CALC An airplane in flight is subject to an air resistance force proportional to the square of its speed v. But there is an additional resistive force because the airplane has wings. Air flowing over the wings is pushed down and slightly forward, so from Newton’s third law the air exerts a force on the wings and airplane that is up and slightly backward ( Fig. P6.94 ). The upward force is the lift force that keeps the airplane aloft, and the backward force is called induced drag. At flying speeds, induced drag is inversely proportional to υ 2 , so the total air resistance force can be expressed by F sir = α υ 2 + β / υ 2 . where α and β are positive constants that depend on the shape and size of the airplane and the density of the air. For a Cessna 150, a small single-engine airplane, α = 0.30 N • s 2 /m 2 and β = 3.5 × 10 5 N • m 2 /s 2 . In steady flight, the engine must provide a forward force that exactly balances the air resistance force, (a) Calculate the speed (in km/h) at which this airplane will have the maximum range (that is. travel the greatest distance) for a given quantity of fuel, (b) Calculate the speed (in km/h) for which the airplane will have the maximum endurance (that is, remain in the air the longest time).
CALC An airplane in flight is subject to an air resistance force proportional to the square of its speed v. But there is an additional resistive force because the airplane has wings. Air flowing over the wings is pushed down and slightly forward, so from Newton’s third law the air exerts a force on the wings and airplane that is up and slightly backward ( Fig. P6.94 ). The upward force is the lift force that keeps the airplane aloft, and the backward force is called induced drag. At flying speeds, induced drag is inversely proportional to υ 2 , so the total air resistance force can be expressed by F sir = α υ 2 + β / υ 2 . where α and β are positive constants that depend on the shape and size of the airplane and the density of the air. For a Cessna 150, a small single-engine airplane, α = 0.30 N • s 2 /m 2 and β = 3.5 × 10 5 N • m 2 /s 2 . In steady flight, the engine must provide a forward force that exactly balances the air resistance force, (a) Calculate the speed (in km/h) at which this airplane will have the maximum range (that is. travel the greatest distance) for a given quantity of fuel, (b) Calculate the speed (in km/h) for which the airplane will have the maximum endurance (that is, remain in the air the longest time).
CALC An airplane in flight is subject to an air resistance force proportional to the square of its speed v. But there is an additional resistive force because the airplane has wings. Air flowing over the wings is pushed down and slightly forward, so from Newton’s third law the air exerts a force on the wings and airplane that is up and slightly backward (Fig. P6.94). The upward force is the lift force that keeps the airplane aloft, and the backward force is called induced drag. At flying speeds, induced drag is inversely proportional to υ2, so the total air resistance force can be expressed by Fsir = α υ2 + β/υ2. where α and β are positive constants that depend on the shape and size of the airplane and the density of the air. For a Cessna 150, a small single-engine airplane, α = 0.30 N • s2/m2 and β = 3.5 × 105 N • m2/s2. In steady flight, the engine must provide a forward force that exactly balances the air resistance force, (a) Calculate the speed (in km/h) at which this airplane will have the maximum range (that is. travel the greatest distance) for a given quantity of fuel, (b) Calculate the speed (in km/h) for which the airplane will have the maximum endurance (that is, remain in the air the longest time).
Consider the situation in the figure below; a neutral conducting ball hangs from the ceiling by an insulating string, and a charged insulating rod is going to be placed nearby.
A. First, if the rod was not there, what statement best describes the charge distribution of the ball?
1) Since it is a conductor, all the charges are on the outside of the ball. 2) The ball is neutral, so it has no positive or negative charges anywhere. 3) The positive and negative charges are separated from each other, but we don't know what direction the ball is polarized. 4) The positive and negative charges are evenly distributed everywhere in the ball.
B. Now, when the rod is moved close to the ball, what happens to the charges on the ball?
1) There is a separation of charges in the ball; the side closer to the rod becomes positively charged, and the opposite side becomes negatively charged. 2) Negative charge is drawn from the ground (via the string), so the ball acquires a net negative charge. 3)…
answer question 5-9
Chapter 6 Solutions
University Physics with Modern Physics (14th Edition)
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