Bucket launched into cloud of star dust.

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Homework Help Overview

The discussion revolves around a physics problem involving a bucket launched into a cloud of star dust. The problem explores the dynamics of the bucket as it collects dust, affecting its mass and velocity over time. Participants are tasked with deriving the position of the bucket as a function of time, x=x(t), while considering the conservation of momentum and energy in an inelastic collision context.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the momentum of the bucket and the dust, with attempts to derive equations governing the system's behavior. Questions arise regarding the assumptions made about external forces and the implications of inelastic collisions on energy conservation. Some participants express confusion about the behavior of x(t) as time approaches infinity.

Discussion Status

There is ongoing exploration of the problem with various approaches being discussed. Some participants have provided equations and attempted to derive relationships between variables, while others question the validity of assumptions and the implications of their findings. The discussion remains open with no explicit consensus reached.

Contextual Notes

Participants are navigating the complexities of the problem, including the effects of dust accumulation on the bucket's mass and the resulting changes in motion. The nature of the collision is noted as inelastic, which raises questions about energy conservation in the context of the problem.

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Homework Statement



An empty bucket (mass M, area A) is launched with velocity v0 from a space station into a cloud of dust (density ρ). As the bucket moves through the dust it will collect dust in it until the bucket comes to a stop. Solve the place of the bucket x=x(t).

2. The attempt at a solution

Okay. Here is my attempt to solve this.

momentum of the bucket dp = v*dm + dv*m.

As a particle of dust with mass dm collides with the bucket its momentum changes by u*dm, where u=-v is the change of the velocity of the particle. On the other hand the change in momentum of the particle has to be the same as the change in momentum of the bucket. So...

dp = u*dm = -v*dm
2*v*dm+m*dv=0
1/v*dv = -2/m*dm
Let's integrate v=v0...v, m=M..m
ln(v0/v) = -2*ln(m/M)
--->
v = v0*(M/m)On the other hand mass of the bucket M will change by
m(x) = M + A*ρ*x
where x is the length of traveled distance.

and this coupled with the equation of velocity we get.
dx/dt = v0*(1+ρ*A*x/M)^-2
v0*dt = (1+ρ*A*x/M)^2 * dx
Lets integrate again t=0..t x=0..x and we get

v0*t = x + k*x^2 + 1/3*k^2*x^3 where k=ρ*A/M

Now by solving x, which I'm not going to do here, we get x=x(t)
Have I done this right? Is there simplier way to do this?
 
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Let's say

total momentum of the whole system is P(t) at some time t.

so

P(t)=mv

P(t+dt)=(m+dm)(v+dv)

dP=P(t+dt)-P(t)=(m+dm)(v+dv)-mv=mv+mdv+dmv+dmdv-mv=mv+dmv

dmdv is very small,so we can neglect it

dP=Fdt=mdv+dmv becase there's no external force on this system we put F=0

dm=\rho Avdt\Rightarrow m(t)=M+\rho Ax

mdv=-dmv

\frac{v(t)}{v_0}=\frac{M_0}{m(t)}

v(t)(M+\rho Ax)dt=M_0v_0dt

\int(M+\rho Ax)dx=\int M_0v_0dt

Mx(t)+\frac{\rho Ax(t)^2}{2}=M_0v_0t
 
azatkgz said:
Mx(t)+\frac{\rho Ax(t)^2}{2}=M_0v_0t

So let's solve x(t):
x(t)=\frac{-M_0+\sqrt{M_0^2+2\rho AM_0v_0t}}{\rho A}

and v(t):
v(t)=\frac{dx}{dt}=\frac{M_0v_0}{\sqrt{M_0^2+2\rho AM_0v_0t}}


v(t)\to0 when t\to\infty as it should. But

x(t)\to\infty when t\to\infty doesn't make sense. It is obvious that the bucket will come to a stop at a some finite point x.
 
azatkgz said:
Let's say

dP=Fdt=mdv+dmv becase there's no external force on this system we put F=0

Is it sure we can say that there is no external forces on the bucket? What about the particles hitting the bucket? Couldn't the hitting be considered as an external force?
 
If particles are hitting him ,then bucket also is hitting them.So total force in bucket-particle system is zero.
 
Okay. What about conservation of energy?
Shouldn't E=\frac{1}{2}M_0v_0^2=\frac{1}{2}(M_0+\rho Ax(t))(v(t))^2 with all values of t.

But when x(t) and v(t) solved from Mx(t)+\frac{\rho Ax(t)^2}{2}=M_0v_0t are put into
E=\frac{1}{2}(M_0+\rho Ax(t))(v(t))^2

We get
E=\frac{1}{2}M_0v_0^2(m_0^2+2\rho AM_0v_0t)^{-\frac{1}{2}}

So something is not right with the solution.

Well on the other hand there are the same problems with solution
v_0t = x + kx^2 + /frac{1}{3}k^2x^3 where k=/rho A/M.
 
deccard said:
Okay. What about conservation of energy?
Shouldn't E=\frac{1}{2}M_0v_0^2=\frac{1}{2}(M_0+\rho Ax(t))(v(t))^2 with all values of t.

Ah! Of course it shouldn't! The collision is inelastic so kinetic energy is not preserved. But still it bothers me that
x(t)\to\infty when t\to\infty. I don't understant it!
 

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