Albert's skydive

In another reality Albert and his friend Bernard are on a plane. Naturally, as most centenarians, they are playful and always ready to fool around. Prankster Bernard pushes Albert out of the plane. While still laughing he states: " Let v ( t ) v(t) be the speed of Albert at time t t . Without parachute, the change in speed between two instants is given by

v ( t + d t ) v ( t ) = g d t μ v ( t ) d t v\left( t+dt \right) \quad -\quad v(t)\quad =\quad gdt\quad -\quad \mu v(t)dt "

where, d t dt is an infinitesimal increment of time, μ \mu is the friction coefficient resulting from Albert's shape and mass, g g is the acceleration of gravity.

Find v M { v }_{ M } , the terminal speed, and Evaluate the quantity v / v M v/{ v }_{ M } at t t = 10s.

Data: μ \mu = 0.18 { s }^{ -1 } ; g g = 4.2 m . s 2 { m.s }^{ -2 } ; v ( 0 ) = v 0 = 0 m . s 1 v(0)={ v }_{ 0 }=0 \ m.{ s }^{ -1 } .

Assumptions: g g , the acceleration of gravity is considered constant.


The answer is 0.83.

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1 solution

Robin P
Jun 6, 2015

Here's one way to solve this problem. We start with Bernard's statement:

(1) v ( t + d t ) v ( t ) = g d t μ v ( t ) d t \quad v(t+dt)\quad -\quad v(t)\quad =\quad gdt\quad -\quad \mu v(t)dt

We can rearrange (1) by dividing both sides by the increment 'dt'

(2) v ( t + d t ) v ( t ) d t = g μ v ( t ) \quad \frac { v(t+dt)-v(t) }{ dt } \quad =\quad g\quad -\quad \mu v(t)

taking the limit as 'dt' goes to 0, (2) yields (3) which is a first-order Ordinary Differential Equation:

(3) d v d t = g μ v ( t ) \quad \frac { dv }{ dt } \quad =\quad g\quad -\quad \mu v(t)

We want to solve for v ( t ) v(t) : First we look for a general solution (i.e a solution to the homogenous equation E H { E }_{ H } )

( E H ) d v d t + μ v ( t ) = 0 { E }_{ H }) \quad \frac { dv }{ dt } \quad +\quad \mu v(t)\quad =\quad 0

We're looking for a function which first derivative is equal the same function times another function (here μ -\mu is a constant function).

Since \frac { d }{ dt } { e }^{ f(t) }\quad =\quad f'(t){ e }^{ f(t) } exponentials are known to have this property.

Therefore { v }_{ H }(t)\quad =\quad A{ e }^{ M(t) },\quad with\quad M(t)\quad =\quad \int _{ 0 }^{ t }{ -\mu dt }

So the general solution to ( E H { E }_{ H } ) is

v H ( t ) = A e μ t { v }_{ H }(t)\quad =\quad A{ e }^{ -\mu t } , where 'A' is a constant defining the initial conditions of the system.

Now all we have to do is to find a particular solution to (3) , you should always look for a constant solution first. Here a constant solution exists:

v p ( t ) = g μ { v }_{ p }(t)\quad =\quad \frac { g }{ \mu }

The complete solution is the sum of the general and particular solutions:

v ( t ) = g μ + A e μ t v(t)\quad =\quad \frac { g }{ \mu } +\quad A{ e }^{ -\mu t }

Now requiring that v ( 0 ) = v 0 = 0 v(0)={ v }_{ 0 }=0 implies A = g μ A=\frac { -g }{ \mu }

So v ( t ) = g μ ( 1 e μ t ) v(t)=\frac { g }{ \mu } (1-{ e }^{ -\mu t })

The terminal speed, v M { v }_{ M } , is given by

v M = l i m t + v ( t ) = g μ { v }_{ M }\quad =\quad \underset { t\rightarrow +\infty }{ lim } v(t)\quad =\quad \frac { g }{ \mu }

And so we obtain the ratio between the speed and the terminal speed:

v v M ( t ) = 1 e μ t \frac { v }{ { v }_{ M } } (t)\quad =\quad 1-{ e }^{ -\mu t }

Which when evaluated at t=10s gives:

v v M \frac { v }{ { v }_{ M } } \quad = 0.83 \boxed{0.83}

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