How Much Force Must a Fireman Exert to Hold a Steadily Ejecting Hose?

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To determine the force a fireman must exert to hold a steadily ejecting hose, the discussion revolves around calculating the momentum change of water flowing through the hose. The hose has a nozzle area of 5 cm² and a cross-sectional area of 360 cm², with water ejected at 25 m/s and a flow rate of 12 L/s. The initial calculations suggest that the water travels at varying speeds within the hose, with the final force calculated as 296 N. However, there is some confusion regarding the mass flow rate and the impact of changing velocities on the overall force required. Ultimately, the conversation emphasizes the importance of using conservation of momentum to accurately assess the force exerted by the fireman.
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The question states: A firemans hose has a nozzle of area 5cm^2 and the hose has a cross sectional area of 360cm^2. The hose ejects water at 25m/s and at a rate of 12L/s What is the force that the fireman must exert to keep the hose steady?

My attempt:

What I have done so far is to calculate the speed of water as it travels through the parts of the hose.

In the nozzle it travels at 24m/s (12000/500) and in the hose it is traveling at (12000/36000) = 0.33ms^-1, and as it is ejected, it is traveling at 25m/s.

So it goes from traveling at 0.33m/s to 24m/s to 25m/s. Hence, the force is
m(v-u)/t = 12kg/s * (25-0.33) = 296N​

So the fireman exerts a force of 296N in the direction of the flow of water.

Is this correct? It seems to simplistic to ignore the 24m/s in the nozzle, yet it seems to work.
 
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This question is to do with momentum. Try and use the conservation of momentum to find the force the firefighter must exert on the hose to steady himself. You know the volume of water being ejected so its easy to find the mass. Also think of the time dependence of the mass.
 
Sorry, but I don't understand what you're getting at. What was wrong with the original approach?
 
zaguar said:
Sorry, but I don't understand what you're getting at. What was wrong with the original approach?

How is m=12kg/s?
The mass flow rate will depend on the cross section of the hose and the velocity. So, it won't be constant.

More specifically \dot{m} = \rho A v, where \dot{m} is the mass flow rate.

What Kurdt says, is to find the difference in the momentum entering and leaving the hose. You can find the force from that.
 
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Isn't that what I did?

Isn't the flow rate always going at 12L/s and the velocity changing, so that there is always 12 litres of water going through the pipe per second, but the speed is different in different parts of the pipe?

So the water is traveling at 0.33m/s in the hose, and exiting at 25m/s. If it is doing that, F=(mv-mu)/t=12*(25-0.33)=296N
 
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