A seaplane of total mass m lands on a lake with initial speed v i i ^ . The only horizontal force on it is a resistive force on its pontoons from the water. The resistive force is proportional to the velocity of the seaplane: R → = − h v → . Newton’s second law applied to the plane is − b v i ^ = m ( d v / d t ) i ^ . From the fundamental theorem of calculus, this differential equation implies that the speed changes according to ∫ v i v d v v = − b m ∫ 0 t d t (a) Carry nut the integration to determine the speed of the seaplane as a function of time. (b) Sketch a graph of the speed as a function of time. (c) Does the seaplane come to a complete stop after a finite interval of time? (d) Does the seaplane travel a finite distance in stopping?
A seaplane of total mass m lands on a lake with initial speed v i i ^ . The only horizontal force on it is a resistive force on its pontoons from the water. The resistive force is proportional to the velocity of the seaplane: R → = − h v → . Newton’s second law applied to the plane is − b v i ^ = m ( d v / d t ) i ^ . From the fundamental theorem of calculus, this differential equation implies that the speed changes according to ∫ v i v d v v = − b m ∫ 0 t d t (a) Carry nut the integration to determine the speed of the seaplane as a function of time. (b) Sketch a graph of the speed as a function of time. (c) Does the seaplane come to a complete stop after a finite interval of time? (d) Does the seaplane travel a finite distance in stopping?
Solution Summary: The author explains the expression for the speed of the seaplane and the force equation using Newton's second law.
A seaplane of total mass m lands on a lake with initial speed
v
i
i
^
. The only horizontal force on it is a resistive force on its pontoons from the water. The resistive force is proportional to the velocity of the seaplane:
R
→
=
−
h
v
→
. Newton’s second law applied to the plane is
−
b
v
i
^
=
m
(
d
v
/
d
t
)
i
^
. From the fundamental theorem of calculus, this differential equation implies that the speed changes according to
∫
v
i
v
d
v
v
=
−
b
m
∫
0
t
d
t
(a) Carry nut the integration to determine the speed of the seaplane as a function of time. (b) Sketch a graph of the speed as a function of time. (c) Does the seaplane come to a complete stop after a finite interval of time? (d) Does the seaplane travel a finite distance in stopping?
Part C
Find the height yi
from which the rock was launched.
Express your answer in meters to three significant figures.
Learning Goal:
To practice Problem-Solving Strategy 4.1 for projectile motion problems.
A rock thrown with speed 12.0 m/s and launch angle 30.0 ∘ (above the horizontal) travels a horizontal distance of d = 19.0 m before hitting the ground. From what height was the rock thrown? Use the value g = 9.800 m/s2 for the free-fall acceleration.
PROBLEM-SOLVING STRATEGY 4.1 Projectile motion problems
MODEL: Is it reasonable to ignore air resistance? If so, use the projectile motion model.
VISUALIZE: Establish a coordinate system with the x-axis horizontal and the y-axis vertical. Define symbols and identify what the problem is trying to find. For a launch at angle θ, the initial velocity components are vix=v0cosθ and viy=v0sinθ.
SOLVE: The acceleration is known: ax=0 and ay=−g. Thus, the problem becomes one of…
Phys 25
Chapter 6 Solutions
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