Particle thrown straight up, need to find velocity

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Homework Help Overview

The discussion revolves around a particle of mass m that is thrown upward with an initial velocity v0. The forces acting on the particle include gravity and a drag force proportional to the square of the velocity, described by b*v2. Participants are attempting to derive the velocity as a function of time while navigating the complexities introduced by the drag force.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the application of Newton's second law and the relationship between acceleration and velocity. There are discussions about the correct signs for forces acting on the particle, the nature of acceleration as it relates to velocity, and the formulation of a differential equation to express the problem.

Discussion Status

Some participants have made progress in formulating the problem as a differential equation and have attempted to separate variables for integration. There is a recognition of the complexity involved in integrating the resulting expressions, and guidance has been offered regarding the separation of variables and the integration process.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can use or the methods they can apply. There is also an acknowledgment that the derived velocity function is only valid for the upward motion of the particle, and the implications of downward motion are noted but not fully explored.

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Ok so I have this particle of mass m that is thrown upward with initial velocity [tex]v_{0}[/tex]. Now there is a downward force due to gravity as well as a square-law drag force described by b*v^2 where b is some constant. I need to find the velocity as a function of time.

Any help is appreciated!
 
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Mugged said:
Ok so I have this particle of mass m that is thrown upward with initial velocity [tex]v_{0}[/tex]. Now there is a downward force due to gravity as well as a square-law drag force described by b*v^2 where b is some constant. I need to find the velocity as a function of time.

Any help is appreciated!

Open your textbook and read the section on Newton's 2nd law
 
heres what i have so far:

F = ma = mg + bv^2

a = g + (b*v^2)/(m)

then i have the kinematic equation:
V = V0 +at

so i plug in my acceleration and then i get the following:

V = V0 + (g + (b*v^2)/(m) ) t

but i need to solve for V and I am not sure how to algebraically move V to one side? I am stuck
 
Mugged said:
heres what i have so far:

F = ma = mg + bv^2

a = g + (b*v^2)/(m)

Do the +/- signs make sense for that? When the particle is moving upwards, the drag force should be downwards and vice versa.

then i have the kinematic equation:
V = V0 +at

That equation is for constant acceleration problems. Your acceleration depends on velocity (thanks to the drag force) and isn't constant. What is the more general relationship between acceleration and velocity?

]
 
oh ok,

so then i should have a = g - (b*v^2)/(m) with g = -9.8 m/s^2

this is while the particle is moving upwards.

as for a general acceleration to velocity relationship, I am not quite sure what you mean. The only other one i can think of is if i differentiated velocity with respect to time i would get acceleration with respect to time.

so since i have acceleration above, you're saying i should integrate to get velocity? if that's correct, i still have no idea how to integrate the right hand side of my above equation

well if i was doing differential equations, it would look something like this:

V' = g - (b*V^2)/(m)

but, I am terrible at dif eq, so id need help here too
 
Mugged said:
oh ok,

so then i should have a = g - (b*v^2)/(m) with g = -9.8 m/s^2

this is while the particle is moving upwards.

If your convention is that v is positive when the particle is moving upwards and negative when it is moving downwards, then yes, that's correct. Similarly, once the particle starts moving downwards, you will have [itex]a=g+\frac{bv^2}{m}[/itex]. You can combine these into one expression by using the sign function [itex]\text{sgn}(v)\equiv \frac{v}{|v|}[/itex] :

[tex]a= g - \text{sgn}(v)\frac{bv^2}{m}[/tex]

The only other one i can think of is if i differentiated velocity with respect to time i would get acceleration with respect to time.

Yes, in other words you have a differential equation:

[tex]\frac{dv}{dt}= g - \text{sgn}(v)\frac{bv^2}{m}[/tex][/tex]

i still have no idea how to integrate the right hand side of my above equation

This ODE is separable, surely you know how to solve one of those?
 
[tex] dv= g - \text{sgn}(v)\frac{bv^2}{m} * dt[/tex]

[tex]v = (g - \text{sgn}(v)\frac{bv^2}{m} ) t[/tex]

is this what you meant? but id still like to get v on one side
 
Mugged said:
[tex] dv= g - \text{sgn}(v)\frac{bv^2}{m} * dt[/tex]

[tex]v = (g - \text{sgn}(v)\frac{bv^2}{m} ) t[/tex]

is this what you meant? but id still like to get v on one side

Divide both sides by [tex]g - \text{sgn}(v)\frac{bv^2}{m}[/tex] before you integrate.
 
hey gab, i think i got the answer in the end after i separated, thanks.

by chance, do you have any idea how to find velocity as a function of the displacement?
 
  • #10
Mugged said:
hey gab, i think i got the answer in the end after i separated, thanks.

by chance, do you have any idea how to find velocity as a function of the displacement?

Use your expression for v(t) to integrate and get y(t) and then eliminate "t" from the two expressions.
 
  • #11
that can't be possible..i have something extraordinarily ugly for my velocity function

[tex]v(t) = \sqrt{\frac{mg}{b}} tan ( tan^-1( \sqrt{\frac{b}{mg}}V_{0}) - gt \sqrt{\frac{b}{mg}} )[/tex]

oh by the way gab, this function is only valid for when velocity is in the positive upward direction, i realized in my homework that i don't need to account for the velocity going down.
 
  • #12
That only looks complicated. It's actually just a shifted tan function. Let

[tex]\alpha = \sqrt{\frac{mg}{b}}[/tex]

Note [itex]\alpha[/itex] is just a convenient combination of constants. You can write v(t) as

[tex]v(t) = \alpha \tan(\phi_0-\frac{gt}{\alpha})[/tex]

where [itex]\phi_0 = \tan^{-1}(v_0/\alpha)[/itex], which is also a constant.
 

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