Two-dimensional coupled nonlinear equations of projectile motion with air resistance in the form of quadratic drag are often treated as inseparable and solvable only numerically. However, when they are recast in terms of the angle between the projectile velocity and the horizontal, they become completely uncoupled and possess analytic solutions for projectile velocities as a function of that angle. The equations relating the time and position coordinates to this angle are not integrable in terms of elementary functions but are easy to integrate numerically. Additionally, energy equations explicitly including dissipation terms can be developed as integrals of the equations of motion. One-dimensional numerical integrations can be treated in a pedagogically straightforward way using numerical analysis software or even within a spreadsheet, making this topic accessible to undergraduates. We present this approach with sample numerical results for velocity components, trajectories, and energy-balance of a baseball-sized projectile.

1.
G. W.
Parker
, “
Projectile motion with air resistance quadratic in the speed
,”
Am. J. Phys.
45
(
7
),
606
610
(
1977
).
2.
S.
Ray
and
J.
Fröhlich
, “
An analytic solution to the equations of the motion of a point mass with quadratic resistance and generalizations
,”
Arch. Appl. Mech.
85
,
395
414
(
2015
).
3.
J. C.
Hayen
, “
Projectile motion in a resistant medium. Part
I: Exact solution and properties,” Int. J. Non-Linear Mech.
38
,
357
369
(
2003
).
4.
C. E.
Mungan
, “
Energy-based solution for the speed of a ball moving vertically with drag
,”
Eur. J. Phys.
27
,
1141
1146
(
2006
).
5.
T.
Timberlake
and
J. E.
Hasbun
, “
Computation in classical mechanics
,”
Am. J. Phys.
76
(
4,5
),
334
339
(
2008
).
6.
See the supplementary material at https://www.scitation.org/doi/suppl/10.1119/5.0095643 for the Excel file containing five example RK4 integrations with two embedded, descriptive pdf documents.
7.
Buoyancy effects can be added ex post facto by replacing g of the gravitational force F g = m g j ̂ with g = g 1 ρ f / ρ, where ρ f is the fluid (air) density and ρ is the average projectile density, see Ref. 15.
8.
J.
Pantaleone
and
J.
Messer
, “
The added mass of a spherical projectile
,”
Am. J. Phys.
79
(
12
),
1202
1210
(
2011
).
9.
H.
Erlichson
, “
Maximum projectile range with drag and lift, with particular application to golf
,”
Am. J. Phys.
52
(
4
),
357
362
(
1983
).
10.
J. M.
Davies
, “
The aerodynamics of golf balls
,”
J. Appl. Phys.
20
(
9
),
821
828
(
1949
).
11.
See http://baseball.physics.illinois.edu/aero.html for spin effects and numerous other articles regarding baseball trajectories.
12.
C.
Clanet
, “
Sports ballistics
,”
Annu. Rev. Fluid Mech.
47
(
1
),
455
478
(
2015
).
13.
When the y- and t ̂-direction equations are recast in terms of ϕ, they become the well-known Bernoulli differential equations with solutions given by v y = v x tan ϕ and v = v x sec ϕ, respectively, see Ref. 3.
14.
R.
Clift
,
J. R.
Grace
, and
M. E.
Weber
,
Bubbles, Drops and Particles
(
Academic Press
,
Cambridge
,
1978
), online data at <https://commons.wikimedia.org/wiki/File:CX_SPHERE.png>
15.
P. T.
Timmerman
and
J. P.
van der Weele
, “
On the rise and fall of a ball with linear or quadratic drag
,”
Am. J. Phys.
67
(
6
),
538
546
(
1999
).
16.
J. L.
Bradshaw
, “
Energy equations for projectiles with linear and quadratic drag
,”
Eur. J. Phys.
44
,
025001
(
2023
).

Supplementary Material

AAPT members receive access to the American Journal of Physics and The Physics Teacher as a member benefit. To learn more about this member benefit and becoming an AAPT member, visit the Joining AAPT page.