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).
air is pushed steadily though a forced air pipe at a steady speed of 4.0 m/s. the pipe measures 56 cm by 22 cm. how fast will air move though a narrower portion of the pipe that is also rectangular and measures 32 cm by 22 cm
No chatgpt pls will upvote
13.87 ... Interplanetary Navigation. The most efficient way
to send a spacecraft from the earth to another planet is by using a
Hohmann transfer orbit (Fig. P13.87). If the orbits of the departure
and destination planets are circular, the Hohmann transfer orbit is an
elliptical orbit whose perihelion and aphelion are tangent to the
orbits of the two planets. The rockets are fired briefly at the depar-
ture planet to put the spacecraft into the transfer orbit; the spacecraft
then coasts until it reaches the destination planet. The rockets are
then fired again to put the spacecraft into the same orbit about the
sun as the destination planet. (a) For a flight from earth to Mars, in
what direction must the rockets be fired at the earth and at Mars: in
the direction of motion, or opposite the direction of motion? What
about for a flight from Mars to the earth? (b) How long does a one-
way trip from the the earth to Mars take, between the firings of the
rockets? (c) To reach Mars from the…
Chapter 6 Solutions
University Physics with Modern Physics (14th Edition)
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