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Question: The flow rate of water from a tap of diameter \(1.25cm\) is \(0.48L/\min \). If the coefficient of v...

The flow rate of water from a tap of diameter 1.25cm1.25cm is 0.48L/min0.48L/\min . If the coefficient of viscosity of water is 103Pa.s{{10}^{-3}}Pa.s, what is the nature of the flow of water?

Explanation

Solution

This problem can be solved by using the direct formula for the Reynold’s number in terms of the density, velocity of flow (which can be found from the rate of volume flow), diameter of tap and the coefficient of viscosity. By analyzing Reynold's number, we can find the nature of the flow.

Formula used:
R=ρvdηR=\dfrac{\rho vd}{\eta }
A=πd24A=\pi \dfrac{{{d}^{2}}}{4}
V=AvV=Av

Complete step-by-step answer:
We will find Reynold's number for the flow and therefore, find out the nature of the flow of water.
The Reynold’s number RR for flow of fluid of density ρ\rho and coefficient of viscosity η\eta in a stream of diameter dd and with velocity vv is given by
R=ρvdηR=\dfrac{\rho vd}{\eta } --(1)
The area AA of cross section of a circle of diameter dd is
A=πd24A=\pi \dfrac{{{d}^{2}}}{4} --(2)
The volume VV of liquid flowing per second in a stream of cross section AA is given by
V=AvV=Av --(3)
where vv is the velocity of the flow of the fluid in the stream.
Now, let us analyze the question.
The diameter of the given tap is d=1.25cm=1.25×102md=1.25cm=1.25\times {{10}^{-2}}m (1cm=102m)\left( \because 1cm={{10}^{-2}}m \right)
Let the area of the opening of the circular tap be AA.
Let the velocity of the fluid just after leaving the tap be vv.
The flow rate of water is V=0.48L/min=0.48103m360s=8×106m3/sV=0.48L/\min =0.48\dfrac{{{10}^{-3}}{{m}^{3}}}{60s}=8\times {{10}^{-6}}{{m}^{3}}/s (1L=103m3,1min=60s)\left( \because 1L={{10}^{-3}}{{m}^{3}},1\min =60s \right)
The coefficient of viscosity is η=103Pa.s\eta ={{10}^{-3}}Pa.s.
The density of water is ρ=103kg/m3\rho ={{10}^{3}}kg/{{m}^{3}}.
Let the Reynold’s number for the flow be RR.
Using (1), we get
R=ρvdηR=\dfrac{\rho vd}{\eta } --(4)
Using (3), we get,
V=AvV=Av --(5)
Using (2), we get
A=πd24A=\pi \dfrac{{{d}^{2}}}{4} --(6)
Putting (6) in (5), we get
V=πd24vV=\pi \dfrac{{{d}^{2}}}{4}v
v=4Vπd2\therefore v=\dfrac{4V}{\pi {{d}^{2}}} --(7)
Putting (7) in (4), we get
R=ρdη4Vπd2=4VρηπdR=\dfrac{\rho d}{\eta }\dfrac{4V}{\pi {{d}^{2}}}=\dfrac{4V\rho }{\eta \pi d}
Putting the values of the variables in the above equation, we get
R=4×8×106×103103×π×1.25×102815R=\dfrac{4\times 8\times {{10}^{-6}}\times {{10}^{3}}}{{{10}^{-3}}\times \pi \times 1.25\times {{10}^{-2}}}\approx 815
Hence, we have got Reynold's number for the flow as 815815. A reynold’s number below 20002000 corresponds to smooth laminar flow and since 815<2000815<2000, we can conclude that the nature of the flow of the water from the tap is a smooth laminar flow.

Note: Students must note that the Reynold’s number that we have calculated is for the flow of liquid just after exiting the tap. It may happen that after the liquid falls for a height, the flow becomes turbulent due to the increase in its speed as gravity acts on it. This can also be felt by the students by a simple experiment. They can open the tap of a basin in their house slightly and observe the flow of the water. At first it is smooth but as it falls down, the flow can become turbulent.