Dynamics question- finding m in terms of rho, r and v

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To determine the mass of water ejected per unit time from the toy rocket's nozzle, the mass flow rate can be calculated using the formula ṁ = ρ * A * v, where A is the cross-sectional area of the nozzle (πr²). This results in ṁ = ρ * πr² * v. For the rate of change of momentum of the water, the relevant equation involves the momentum change, which is the product of mass flow rate and velocity, leading to the expression for momentum change as F = ṁ * v. The discussion emphasizes the importance of understanding mass flow rate in fluid dynamics, particularly in applications like rocketry. Overall, the calculations hinge on the relationships between density, area, and velocity.
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Homework Statement


A toy rocket consists of a plastic bottle which is partially filled with water. the space above the water contains compressed air.

At one instant during the flight of the rocket, water is of density\rho is forced through the nozzle of radius r at speed v relative to the nozzle. Determine, in terms of \rho, r and v:

1. the mass of the water ejected per unit time from the nozzle

2. the rate of change of momentum of the water.

Homework Equations



F=ma
\rho=mass/volume
Area of nozzle through which water passes=\pir2

The Attempt at a Solution



This is what I did for part 1:
\rho=m/volume
therefore, m=\rho x volume

RE: area through which water exits:\pir2
therefore, m=(\pir2)(\rho) x length

I think the mass per unit time means divide by time?

m/t=[(\pir2)(\rho) x length]/t

I do not know how to do part 2..
 
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Ok, well for number 1, i think you approached it a little too complicated. When the want mass per unit time, that is the mass flowrate. Volume per unit time is the volumetric flowrate. Mass flow rate is often used for gasses in rockets for example, because even if the density changes, the mass doesn't, whereas, the volume will change with changing density.

That aside,
m=rho*V
Q=Av (Volumetric flowrate is Area of nozzle times velocity of fluid, v, with a constant density)
mass flowrate, \dot{m}=rho*Q or rho*A*v
So mass flowrate, \dot{m}=\frac{dm}{dt}=rho*\pir²*v
where \frac{dm}{dt} is change in mass with time, or mass flowrate.
 
For part two, you need the relevant equations for momentum, what are they?
 
Thanks, I got it.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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