I need a little help attacking a problem

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To analyze the skydiver's jump, the initial conditions include a velocity of 100 mph and a position of 2000 m, with gravity acting at -9.81 m/s². Air friction can be calculated using the drag force equation F(v) = cρAv², where A is the surface area and ρ is air density. The acceleration can be expressed as a(v) = (cρA/m)v², requiring integration to find velocity as a function of time. It's essential to normalize units and recognize that air resistance acts in the opposite direction to velocity. Solving the resulting second-order differential equations will provide insights into changes in acceleration and velocity throughout the fall.
arkssd
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hello,

what would be the best way to approach this problem

A skydiver is jumping out of a plane at :

Initial velocity = 100 mph

Initial position = 2000 m

acceleration due to gravity = -9.81

I need help finding air friction at different positions, change in acceleration and change in velocity ?

i think u calculate air friction
A= f * v * v(abs) * cd

A= acceleration

f= atmospheric pressure

v= velocity

s= surface area

cd= drag coefficient
 
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Start off with Newton's 2nd Law (For constant mass) in scalar form:

\sum_{i=1}^{n} F_{i} = ma

rewrite it as

\sum_{i=1}^{n} F_{i} = m \frac{dv}{dt}

or

\sum_{i=1}^{n} F_{i} = m \frac{d^{2} x}{dt^{2}}

And solve the ODEs formed
 
arkssd said:
hello,

what would be the best way to approach this problem

A skydiver is jumping out of a plane at :

Initial velocity = 100 mph

Initial position = 2000 m

acceleration due to gravity = -9.81

I need help finding air friction at different positions, change in acceleration and change in velocity ?

i think u calculate air friction
A= f * v * v(abs) * cd

A= acceleration

f= atmospheric pressure

v= velocity

s= surface area

cd= drag coefficient

the general form of that equation looks familiar, but isn't it actually:

F(v) = c \rho A v^2

where A[/tex] is the surface area? Acceleration would then be:<br /> <br /> a(v) = \frac{c \rho A v^2}{m} = \frac{c \rho A}{m} ({\frac{dx}{dt}})^2<br /> <br /> integrating with respect to time will give the velocity as a function of time, but this is a 2nd order DE so you need to solve the DE and plug in your initial value conditions.
 
Not really II-nd order.Use Newton's second law in vector and the definition of linear momentum.

Daniel.
 
Normalize your units first off.
 
There's no atmospheric pressure in the drag force,just the air's density...

Daniel.
 
quetzalcoatl9 said:
the general form of that equation looks familiar, but isn't it actually:

F(v) = c \rho A v^2

where A[/tex] is the surface area? Acceleration would then be:<br /> <br /> a(v) = \frac{c \rho A v^2}{m} = \frac{c \rho A}{m} ({\frac{dx}{dt}})^2<br /> <br /> integrating with respect to time will give the velocity as a function of time, but this is a 2nd order DE so you need to solve the DE and plug in your initial value conditions.
<br /> Nope, this is false; air resistance always works in the opposite direction of the velocity; that&#039;s why you need the absolute value sign here.
 
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