What Does the Constant 'b' Represent in the Drag Force Equation?

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Homework Help Overview

The discussion revolves around the drag force equation, specifically the constant 'b' in the context of objects in free fall experiencing drag. Participants explore the implications of different forms of the drag force and the resulting differential equations governing motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants analyze the drag force equation F=-bv^2 and its implications on motion, questioning the correct form of the differential equation. Some participants explore variations of the drag force, such as F=-2v, and discuss the effects of ignoring gravity. There are attempts to derive solutions for velocity and to interpret graphical representations of motion.

Discussion Status

The discussion is active, with participants providing various interpretations and analyses of the drag force and its effects on motion. Some participants have offered insights into the mathematical solutions, while others are questioning the assumptions made regarding the drag force and gravity. There is no explicit consensus on the interpretations or solutions presented.

Contextual Notes

Participants are working under the assumption of neglecting gravity in certain scenarios, which influences the form of the equations being discussed. The nature of the drag force is also under scrutiny, with different values for 'b' being considered.

UrbanXrisis
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free fall with drag force

If the equation F=-bv^2 describes the drag force of an object...then the differential equation for the object's motion would be:

dv/dt= -g+bv/m

or is it...

dv/dt= g-bv/m

After solving the equation, should I get...
V=mg/b[1-e^(-bt/m)]

Also, does this look like the position v time graph of the object?
http://home.earthlink.net/~urban-xrisis/phy001.gif
 
Last edited by a moderator:
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Ok i'll do the analysis.

Forces acting on a body falling.
Down positive (Using resistive force proportional to the speed)

We got a first order DE

[tex]mg - bv = m \frac{dv}{dt}[/tex]

To not get into much detail, this type of DE

[tex]\frac{dy}{dt} = ay - b[/tex]

Has the following solution

[tex]y = \frac{b}{a} + ce^{at}[/tex]

For an initial value, to find C.

[tex]y = \frac{b}{a} + [y_{o} - \frac{b}{a}]e^{at}[/tex]

Thus for our case the solution is

[tex]v = \frac{mg}{b} + [v_{o} - \frac{mg}{b}]e^{-\frac{bt}{m}}[/tex]

If we arrange the terms and [itex]v_{o} = 0[/itex]

[tex]v = \frac{mg}{b} - \frac{mg}{b}e^{-\frac{bt}{m}}[/tex]

[tex]v = \frac{mg}{b}(1 - e^{-\frac{bt}{m}})[/tex]
 
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instead of F=-bv^2, what if F=-2v? The question tells me to ignore the effects of gravity in this problem. Would the DE then be dv/dt= 2v/m?

Since f=bv...and b=-2

dv/dt= g-bv/m
dv/dt= g-(-2)v/m
the question asks to ignore gravity...
dv/dt= -(-2)v/m
dv/dt= 2v/m
 
If we ignore gravity, then indeed our Newtonian analysis will be

The Object is falling, and the air drag is in the opposite direction
Down positive.

[tex]m\frac{dv}{dt} = -bv[/tex]

[tex]\frac{dv}{dt} = \frac{-bv}{m}[/tex]

Solving this:

[tex]\frac{dv}{dt} = \frac{-bv}{m}[/tex]

[tex]\frac{dv}{v} = \frac{-b}{m}dt[/tex]

[tex]\int_{v_{o}}^{v} \frac{dv}{v} = \int_{0}^{t} \frac{-b}{m}dt[/tex]

[tex]\ln |v|]_{v_{o}}^{v} = \frac{-b}{m}t]_{0}^{t}[/tex]

For [itex]v_{o} = 0[/itex]

[tex]ln |v| = \frac{-b}{m}t[/tex]

[tex]v = e^{\frac{-b}{m}t}[/tex]
 
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UrbanXrisis said:
Also, does this look like the position v time graph of the object?
http://home.earthlink.net/~urban-xrisis/phy001.gif

Does this look correct?
 
Last edited by a moderator:
Cyclovenom said:
If we ignore gravity, then indeed our Newtonian analysis will be

The Object is falling, and the air drag is in the opposite direction
Down positive.

[tex]m\frac{dv}{dt} = -bv[/tex]

[tex]\frac{dv}{dt} = \frac{-bv}{m}[/tex]

Solving this:

[tex]\frac{dv}{dt} = \frac{-bv}{m}[/tex]

[tex]\frac{dv}{v} = \frac{-b}{m}dt[/tex]

[tex]\int_{v_{o}}^{v} \frac{dv}{v} = \int_{0}^{t} \frac{-b}{m}dt[/tex]

However, the retarding force is not F=bv, it is F=-2v as stated above. Correct me if I’m wrong, but isn’t [tex]\frac{dv}{dt} = \frac{-bv}{m}[/tex] for when F=bv? Should it be [tex]\frac{dv}{dt} = \frac{2v}{m}[/tex] ?
 
Sure, just substitute b with 2, and for the graphic, It looks rather odd to me, but maybe someone else can find it the physical meaning.
 
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my graph represents the object accelerating and to at point where it has constant velocity because of the drag force

or should it look something like this...
http://home.earthlink.net/~urban-xrisis/phy002.gif
 
Last edited by a moderator:
the graphic looks better now, and i added the extra solve steps for neglecting gravity.
 
  • #10
what is b in this equation
 

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