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Module 3.1 Modeling Falling and Skydiving

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1 Module 3.1 Modeling Falling and Skydiving
Angela B. Shiflet and George W. Shiflet Wofford College © 2014 by Princeton University Press

2 Model falling ball Simplification Variables and equations No friction
Position, s Velocity, v(t) = ds/dt Acceleration, a(t) = dv/dt Acceleration due to gravity = m/sec2

3 Model falling ball

4 Refinement of model - friction
Forces acting on body Weight Newton’s Second Law, F = ma F , force acting on body m, mass of body a, acceleration unit for force - Newton (N) or kg m / sec2

5 Model falling ball Forces acting on body Kinetic friction or drag
Estimates Stokes' friction, F = kv (for a very small object moving slowly through fluid) k, kg/sec, constant of proportionality v in m/sec, velocity. Newtonian friction, F = 0.5CDAv2 (for a large object moving faster through a fluid) C, constant of proportionality (coefficient of drag or drag coefficient); dimensionless constant related to the shape of the object D, density of the fluid A, object's projected area in the direction of movement

6 Model falling ball Forces acting on body
Kinetic friction or drag Estimates Stokes' friction, F = kv Newtonian friction, F = 0.5CDAv2 Newtonian friction through air, F = 0.65Av2 (for large objects with C = 1 moving faster through sea-level air where the density of the air is D = 1.29kg/m3 at sea level) A: object’s projected area in direction of movement v: velocity Note that F = 0.5CDAv2 can be rewritten as F = -0.5CDAv|v| (sine the drag force is in the opposite direction as v).

7 Model falling ball with air friction
Figure 3.1.4

8 Equation Set 3.1.1 DE: m*dv/dt = -m*g + 0.65*A*v2, v(0) = 0; this is
a non-linear DE.

9 Equation Set 3.1.1

10 Model skydiving We ignore changes of air density for simplicity. Note the projected area A is not a constant here as in the falling ball example.

11 Model skydiving The model for a skydive out of a helicopter has two phases, one where the person is in a free fall (A ~ 0.4 m2) and the other after the parachute opens, when the larger surface area results in more air resistance (A ~ 28 m2). Assume the pull of the ripcord is at 1000 m above the ground, and the parachute fully opens instantaneously.

12 Model skydiving


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