Terminal velocity with an initial velocity?

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Discussion Overview

The discussion revolves around the concept of terminal velocity, particularly in the context of an object starting with an initial velocity. Participants explore the time it takes to reach terminal velocity and the forces acting on a falling object, including drag and gravity. The conversation includes mathematical modeling and differential equations related to the motion of falling objects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant asks how to calculate the time to reach terminal velocity from an initial velocity, referencing a specific webpage.
  • Another participant notes that terminal velocity is approached asymptotically, suggesting that one can consider the time to reach a certain percentage of terminal velocity.
  • A different participant expresses confusion about the concept of never truly reaching terminal velocity and requests a more detailed explanation.
  • Concerns are raised about the validity of the referenced webpage, with a participant claiming it confuses free-fall acceleration with drag acceleration, while acknowledging the drag force is correctly identified.
  • Participants discuss the forces acting on a falling object, including gravity and drag, and present a differential equation to model the motion.
  • One participant mentions that for objects with a large drag-to-mass ratio, such as a skydiver with an open parachute, calculating the time to reach the ground is straightforward since they move at terminal velocity.
  • Another participant provides a simplified explanation of differential equations in the context of modeling the acceleration of a falling object, emphasizing the relationship between gravity and air resistance.
  • A participant explains the process of solving a differential equation through separation of variables, providing a mathematical example.

Areas of Agreement / Disagreement

Participants express differing views on the nature of terminal velocity, with some suggesting it can never be fully reached while others imply practical scenarios where it is effectively achieved. The discussion includes multiple competing perspectives on the mathematical modeling of the problem, and no consensus is reached on the best approach or interpretation.

Contextual Notes

There are limitations regarding the assumptions made about the forces acting on the object, the definitions of terms used, and the mathematical steps involved in solving the differential equations. Some participants express uncertainty about the mathematical concepts discussed.

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As a quick answer, you only approach terminal velocity asymtotically, that is, you could ask when you reach 95% of terminal velocity, but technically when you reach terminal velocity
 
flatmaster said:
As a quick answer, you only approach terminal velocity asymtotically, that is, you could ask when you reach 95% of terminal velocity, but technically when you reach terminal velocity

you mean you can never really reach terminal velocity, everyone keeps telling me that.

But I have a questions that ask when it reaches terminal velocity and how long does it take for the object to fall to the ground.

What's the long answer? lol
 
That page you cyted is no good. He mixed up free-fall acceleration and drag acceleration.

He got the drag force right though.


Fdrag = .5pCAv^2

Where,

v is velocity (m/s)

C is the object's Drag Coefficient.

A is the object's cross sectional area (),

p and is the density of air (assume 1.25 kg/m3)


Ok. What are the forces acting on the object?


F=ma

Gravity and the drag force. Assume up is the positive direction.

.5pCAv^2 - mg = ma


Here, you have a differential equation. Knowing a = dv/dt


B(v)^2 - D = G dv/dt

Is your differential equation to solve with B, D, and G representing new constants
 
In the real world, you can think of it as if you're falling at your terminal velocity after nearly reaching it. It's only mathematical rigor that says you can never reach your terminal velocity.

Calculating the time to reach the ground is easy for something with a large drag to mass ratio (skydiver with open parachute). You're quite simply moving at your terminal velocity. It's simply a constant velocity problem in the vertical (y) direction

where V is your terminal velocity and y is the total height to fall.

V = y/t

t = y * V


However, if you have something with a large terminal velocity, the total time will be longer than this because early in the fall, the object was moving slower than it's terminal velocity
 
flatmaster said:
That page you cyted is no good. He mixed up free-fall acceleration and drag acceleration.

He got the drag force right though.


Fdrag = .5pCAv^2

Where,

v is velocity (m/s)

C is the object's Drag Coefficient.

A is the object's cross sectional area (),

p and is the density of air (assume 1.25 kg/m3)


Ok. What are the forces acting on the object?


F=ma

Gravity and the drag force. Assume up is the positive direction.

.5pCAv^2 - mg = ma


Here, you have a differential equation. Knowing a = dv/dt


B(v)^2 - D = G dv/dt

Is your differential equation to solve with B, D, and G representing new constants

Thank you for your reply.

The terminal velocity is 41.4m/s and its only a height of 200m

Hmmm I'm in high school so I'm not really sure differential equation. Did you just take the derivative?

"A simplified real world example of a differential equation is modeling the acceleration of a ball falling through the air (considering only gravity and air resistance). The ball's acceleration towards the ground is the acceleration due to gravity minus the acceleration due to air resistance. Gravity is a constant but air resistance is proportional to the ball's velocity. This means the ball's acceleration is dependent on its velocity. Because acceleration is the derivative of velocity, solving this problem requires a differential equation."
 
A differential equation is an equation where the derivative of a variable depends on that same variable in one way or another.

For example:
[tex]\frac{dy}{dx} = 2y[/tex]

What you can do in this case is called separation of variables: you bring all the y's to the left and all the x's to the right (or the other way around):
[tex]\frac{dy}{y} = 2\, dx[/tex]

Now, you can integrate both sides:
[tex]\int \frac{dy}{y} = \int 2\, dx[/tex]
[tex]\ln y = 2x + C[/tex]

Then you can solve for y = y(x).
 

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