Force of a water flow through a U-shaped pipe

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Homework Help Overview

The discussion revolves around calculating the force required to compensate for the water flow in a U-shaped pipe, where water flows at a speed of 0.75 m/s through a circular cross-section. Participants are exploring concepts related to momentum, pressure, and mass flow rate.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of conservation of momentum and pressure equations, questioning how to separate force from momentum terms. There is an exploration of how momentum enters and exits the pipe over a small time interval, with some participants expressing uncertainty about the implications of this interval on mass flow.

Discussion Status

The discussion is active, with participants attempting to clarify their understanding of momentum and mass flow in the context of the problem. Some guidance has been offered regarding the interpretation of mass flow over time, but no consensus has been reached on the specifics of the calculations or the implications of the small time interval.

Contextual Notes

Participants are grappling with the definitions and implications of mass flow and momentum in a fluid dynamics context, with some expressing confusion about the relationship between mass, time intervals, and the resulting calculations.

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Homework Statement


Water flows at a speed of 0.75 m / s through a U-shaped tube whose cross-section is circular with a radius of 10 mm. How large is the force F to be to compensate for water power on the tube?




Homework Equations


I am not sure. Perhaps;

Pressure=Force/Area
Conservation of momentum
Density = mass/volume

The Attempt at a Solution



I believe that the speed of water flow is the same through the whole pipe but the velocities have different signs in each side of the pipe. Of course the mass is constant.if I use conservation of momentum I will have:

Fdt=m(Δv)=m(v_1-v_2)=m(v-(-v))=2mv

Fdt=2mv. The mass is not given but if we knew the volume we could find it as m=ρV. And how can I separate F from Fdt?

I tried this(wrong);

Fdt=2mv=2m(dx/dt) --->F=2m(d^2x/dt^2)=2ma=0 since velocity is constant.
 
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Find how much momentum enters the pipe over dt, and how much leaves it. The differnce between these two momenta is the impulse.
 
voko said:
Find how much momentum enters the pipe over dt, and how much leaves it. The differnce between these two momenta is the impulse.

Momentum that enters the pipe: mv
Momentum that leaves the pipe: -mv
The difference is then mv-(mv)=2mv=Fdt. I just don't know what to do with dt and mass m.
 
How do you interpret my phrase "how much momentum enters the pipe over dt", with emphasis on "over"?
 
voko said:
How do you interpret my phrase "how much momentum enters the pipe over dt", with emphasis on "over"?

i believe it means during a very small time interval. Which is no different in my imagination. It enters p=mv at the top, whether it is a short or not so short interval. Is that wrong?
 
The question is, how much mass enters over this very small time interval.
 
voko said:
The question is, how much mass enters over this very small time interval.

I am not sure actually. During a very small time interval enters a very small amount of mass and if the time interval --->0 then the amount of mass that enters --->0. But I don't see how this helps...
 
You are right, this does not help at all. You need to be more specific about what this very small amount really is.

Imagine that at some time t you draw a plane perpendicular to the pipe at its entry, and then you let this plane move along the pipe with the flow. At time t + dt, you draw another such plane. These two planes contain your very small amount of mass. What is it in terms of what you are given?
 
voko said:
You are right, this does not help at all. You need to be more specific about what this very small amount really is.

Imagine that at some time t you draw a plane perpendicular to the pipe at its entry, and then you let this plane move along the pipe with the flow. At time t + dt, you draw another such plane. These two planes contain your very small amount of mass. What is it in terms of what you are given?

More specific? Well how about taking the derivative; (dp/dt)dt=dp=2mv which is the same thing as before, nothing new. I'm going in circles here. I think this is the same thing as the idea with the planes, although I do see that the difference will contain the mass.
 
  • #10
You completely ignored the second part of #8. No wonder you are going in circles.
 
  • #11
What is the rate at which mass is flowing through the pipe in kg/sec?
 

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