Introduction to Computational Physics Homework 5: Projectile Motion with Air Resistance, Assignments of Physics

The spring 2009 edition of physics 105 homework #5, focusing on projectile motion in two dimensions under the influence of gravity and air resistance. Students are required to compute the projectile's range, time of flight, and angles of impact for two different values of air resistance, interpolate results, and plot trajectories. Additional problems involve determining the required launch speed to restore the range and finding the maximum range for a given launch speed.

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Pre 2010

Uploaded on 08/18/2009

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PHYS 105: Introduction to Computational Physics
Spring 2009
Homework #5
(Due: May 21, 2009)
1. Do in-class exercise 7.1. Turn in your program (part 2) and three plots (parts 4 and 5), and
clearly state the results you obtain in response to the other questions asked.
2. Consider again a projectile moving in two dimensions under the combined effects of gravity
and air resistance. Initially the projectile is launched from x= 0, y = 0 with speed v0= 100
m/s at an angle of θ0= 60◦to the horizontal. The components of its acceleration are
ax=−β|v|vx,
ay=−g−β|v|vy,
where β= 0.001 (chosen so that the initial acceleration for this value of v0is the same as the
case Îą= 0.1 in problem 1).
(a) Compute the projectile’s range and time of flight (take δt = 0.01, and don’t forget to
interpolate!), and compare them to the results of the ι= 0.1, β = 0 calculation in
problem 1. Plot both trajectories (ι= 0.1, β = 0 and ι= 0, β = 0.001) on the same
graph.
(b) At what angle to the horizontal θ1does the projectile hit the ground in either case in
part (a)? What would θ1be in the absence of air resistance (i.e. ι=β= 0)?
(c) By what factor (to within 1 percent) must the launch speed for ι= 0, β = 0.001 be
increased to restore the range to the ι=β= 0 result?
(d) By varying the value of θ0, determine the maximum range of the projectile for v0= 100
m/s (again with ι= 0, β = 0.001). To what value of θ0(to 1 decimal place) does this
correspond?
(e) For v0= 100 m/s, plot θ1as a function of θ0.
3. Now suppose that the value of βin problem 2 varies with height y, according to the law
β(y) = 0.001e−y/h ,
where h= 500 m (not a very realistic description of Earth’s atmosphere!). How does the
maximum range of the projectile (as computed in problem 2d) change as a result? What if h
= 5 km (a much better approximation to reality)?

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PHYS 105: Introduction to Computational Physics

Spring 2009

Homework

(Due: May 21, 2009)

  1. Do in-class exercise 7.1. Turn in your program (part 2) and three plots (parts 4 and 5), and clearly state the results you obtain in response to the other questions asked.
  2. Consider again a projectile moving in two dimensions under the combined effects of gravity and air resistance. Initially the projectile is launched from x = 0, y = 0 with speed v 0 = 100 m/s at an angle of θ 0 = 60◦^ to the horizontal. The components of its acceleration are

ax = −β |v| vx , ay = −g − β |v| vy ,

where β = 0.001 (chosen so that the initial acceleration for this value of v 0 is the same as the case ι = 0.1 in problem 1).

(a) Compute the projectile’s range and time of flight (take δt = 0.01, and don’t forget to interpolate!), and compare them to the results of the α = 0. 1 , β = 0 calculation in problem 1. Plot both trajectories (α = 0. 1 , β = 0 and α = 0, β = 0.001) on the same graph. (b) At what angle to the horizontal θ 1 does the projectile hit the ground in either case in part (a)? What would θ 1 be in the absence of air resistance (i.e. α = β = 0)? (c) By what factor (to within 1 percent) must the launch speed for α = 0, β = 0.001 be increased to restore the range to the α = β = 0 result? (d) By varying the value of θ 0 , determine the maximum range of the projectile for v 0 = 100 m/s (again with α = 0, β = 0.001). To what value of θ 0 (to 1 decimal place) does this correspond? (e) For v 0 = 100 m/s, plot θ 1 as a function of θ 0.

  1. Now suppose that the value of β in problem 2 varies with height y, according to the law

β(y) = 0. 001 e−y/h^ ,

where h = 500 m (not a very realistic description of Earth’s atmosphere!). How does the maximum range of the projectile (as computed in problem 2d) change as a result? What if h = 5 km (a much better approximation to reality)?