Terminal velocity of a raindrop

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Homework Help Overview

The discussion revolves around the terminal velocity of a raindrop gaining mass as it falls under gravity. The original poster presents a differential equation relating the forces acting on the raindrop, including its changing mass and velocity.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the relationship between mass, velocity, and forces acting on the raindrop, questioning the validity of the equations used. Some suggest finding conditions for constant velocity, while others raise concerns about the assumptions made regarding mass and momentum.

Discussion Status

There is an ongoing examination of the equations presented, with some participants offering alternative perspectives on the treatment of mass and momentum. Several interpretations of the problem are being explored, particularly regarding the effects of buoyancy and drag forces.

Contextual Notes

Participants note that the problem does not provide values for relative velocities or consider all forces acting on the raindrop, which may affect the analysis.

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Homework Statement



A raindrop of initial Mass ##M_0## starts to fall from rest under the influence of gravity. Assume that the drop gains mass from the cloud at a rate proportional to the product of its instantaneous mass and its instantaneous velocity ##\dfrac{dM}{dt} = kMV##, where ##k## is constant. show that speed eventually become constant.

Homework Equations

The Attempt at a Solution



##P_i = M_0v##

##P_f = \left( M_0 + \left(\Delta t \dfrac{dM}{dt}\right) \right)(v + \Delta v)##

therefore ##\Delta P = M_0 \Delta v + v \Delta t\dfrac{dM}{dt}##

Since ##F = \lim_{\Delta t \to 0} \dfrac{\Delta P}{\Delta t}##

Therefore ##F = M_0 \dfrac{dv}{dt} + v \dfrac{dM}{dt}##

Substituting ##\dfrac{dM}{dt} = kMV##,

##F = M_0 \dfrac{dv}{dt} + k M v^2##

The velocity will be constant if the forces are balanced,

therefore, ##Mg = M_0 \dfrac{dv}{dt} + k M v^2##

Now I don't know what to do ? should I solve for ##v## in this differential equation and then find the time at which it would be constant (I tired but it was very messy with lots of constants, I got ##v = \displaystyle u\dfrac{1- \exp(2ku\alpha t)}{\exp(2ku\alpha t) - 2} ## where ##u = \sqrt{h/k}## and ##\alpha = M/M_0##) ?
 
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Actually:
$$F = \frac{d(Mv)}{dt} = M \dfrac{dv}{dt} + v \dfrac{dM}{dt}$$
Then you just need to find the condition that will set ##\dfrac{dv}{dt} = 0##.
 
jack action said:
Actually:
$$F = \frac{d(Mv)}{dt} = M \dfrac{dv}{dt} + v \dfrac{dM}{dt}$$
Then you just need to find the condition that will set ##\dfrac{dv}{dt} = 0##.

But I got ##M_0## instead of ##M##.
 
I know, but it should be the instantaneous mass, not the initial mass:

##P_i = Mv##
##P_f = \left( M + \left(\Delta t \dfrac{dM}{dt}\right) \right)(v + \Delta v)##

With the initial mass ##M_0##, it is only valid for the initial instant as with ##M## it is valid at any moment.
 
jack action said:
I know, but it should be the instantaneous mass, not the initial mass:

##P_i = Mv##
##P_f = \left( M + \left(\Delta t \dfrac{dM}{dt}\right) \right)(v + \Delta v)##

With the initial mass ##M_0##, it is only valid for the initial instant as with ##M## it is valid at any moment.

Then we get,

##Mg = M \dfrac{dv}{dt} + k M v^2##

##g - kv^2 = \dfrac{dv}{dt}##. Therefore at ##g = kv^2##, velocity is constant. Is this fine ?
 
That would be my answer. When ##v= \sqrt{\frac{g}{k}}##, you will have no more acceleration, so it will stay at this speed constantly.
 
and shouldn't the buoyancy and drag forces on the drop be considered ?
 
-
 
Last edited:
  • #10
zwierz said:
It seems to be wrong. This equation does not take in respect that the particles of the fluid in the cloud have nonzero velocity relative to the raindrop and thus those particles bring momentum as they meet the raindrop. For details seehttp://www3.nd.edu/~powers/ame.20231/ajp.1962.pdf
see also http://www.lcurve.org/writings/PT-NewtonsLawsForVariableMass.pdf

But in the question no value of relative velocity is given :).

Nidum said:
and shouldn't the buoyancy and drag forces on the drop be considered ?

:nb):nb)
 
  • #11
zwierz said:
This equation does not take in respect that the particles of the fluid in the cloud have nonzero velocity relative to the raindrop
I agree that the equation F=dp/dt=d(mv)/dt=mdv/dt+vdm/dt is not kosher. It treats mass as something that can change in a closed system.
However, it does give the right answers when the mass entering or leaving the system does so with no momentum in the frame of reference. In this case, we can assume that the moisture being collected had been stationary relative to the ground.
 
  • #12
look here: http://www3.nd.edu/~powers/ame.20231/ajp.1962.pdf
I marked the missed term with the red frame

c3dfb72bc09a.png
 
  • #13
Oh! that is my mistake. In this problem u=0
 
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