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Question: Glycerine flows steadily through a horizontal tube of length \[1.5{\text{ m}}\] and radius \[1.0{\te...

Glycerine flows steadily through a horizontal tube of length 1.5 m1.5{\text{ m}} and radius 1.0 cm1.0{\text{ cm}}. If the amount of glycerine collected per second at one end is 4.0×103  kgs - 14.0 \times {10^{ - 3}}\;{\text{kg}}{{\text{s}}^{{\text{ - 1}}}}, what is the pressure difference between the two ends of the tube ? (Density of glycerine =1.3×103  kgm - 3 = 1.3 \times {10^3}\;{\text{kg}}{{\text{m}}^{{\text{ - 3}}}} and viscosity of glycerine =0.83  Pa  S = 0.83\;{\text{Pa}}\;{\text{S}}). [You may also like to check if the assumption of laminar flow in the tube is correct].

Explanation

Solution

First we convert all the units in SI form, i.e. convert all centimetres to metres. Since, the radius is given, the diameter can be obtained. From Poiseuille's formula V=πP×r48ηlV = \dfrac{{\pi P \times {r^4}}}{{8\eta l}}, and then we calculate the value of pressure. To obtain Reynolds number we use the formula R=4ρVπdηR = \dfrac{{4\rho V}}{{\pi d\eta }}

Complete step by step answer:
Given, length of the horizontal tube, l=1.5  ml = 1.5\;{\text{m}}
Radius of the tube, r=1  cmr = 1\;{\text{cm}}
Glycerine is flowing at a rate of 4.0×103  kgs - 14.0 \times {10^{ - 3}}\;{\text{kg}}{{\text{s}}^{{\text{ - 1}}}}
M=4.0×103  kg/sM = 4.0 \times {10^{ - 3}}\;{\text{kg/s}}
Density of glycerine, ρ=1.3×103  kg/m3\rho = 1.3 \times {10^3}\;{\text{kg/}}{{\text{m}}^3}
Viscosity of glycerine, η=0.83  Pa  S\eta = 0.83\;{\text{Pa}}\;{\text{S}}
Convert all the units in SI form, i.e. convert all centimetres to metres.
Hence,
Radius of the tube, r=1  cm=0.01  mr = 1\;{\text{cm}} = {\text{0}}{\text{.01}}\;{\text{m}}
Diameter of the tube, d=2r=0.02  md = 2r = 0.02\;{\text{m}}
Now, volume of the glycerine per second is obtained by dividing MM
by density of glycerine.
i.e.

V=4×1031.3×103 =3.08×106  m3/s  V = \dfrac{{4 \times {{10}^{ - 3}}}}{{1.3 \times {{10}^3}}} \\\ = 3.08 \times {10^{ - 6}}\;{{\text{m}}^{\text{3}}}{\text{/s}} \\\

For the relation of the rate of flow, apply Poiseuille's formula.
V=πP×r48ηlV = \dfrac{{\pi P \times {r^4}}}{{8\eta l}}; PP is the difference of pressure of the two ends of the tube.
Rearrange the above equation to obtain the value of PP.

P=V8ηlπr4 =3.08×106×8×0.83×1.5π×(0.01)4 =9.8×102  Pa  P = \dfrac{{V8\eta l}} {{\pi {r^4}}} \\\ = \dfrac{{3.08 \times {{10}^{ - 6}} \times 8 \times 0.83 \times 1.5}} {{\pi \times {{\left( {0.01} \right)}^4}}} \\\ = 9.8 \times {10^2}\;{\text{Pa}} \\\

Reynolds number is obtained by the relation,

R=4ρVπdη =4×1.3×103×3.08×106π×0.02×0.83 =0.3  R = \dfrac{{4\rho V}}{{\pi d\eta }} \\\ = \dfrac{{4 \times 1.3 \times {{10}^3} \times 3.08 \times {{10}^{ - 6}}}}{{\pi \times 0.02 \times 0.83}} \\\ = 0.3 \\\

Since, the Reynolds number is 0.30.3.
Therefore, the flow is laminar.

So, the correct answer is “Option A”.

Additional Information:
The Reynolds number is the ratio of inertial forces and viscous forces inside a fluid that, owing to different fluid velocities, is subject to similar spatial movement. As a boundary plate, such as the flowing fluid in the interior of a container, an area in which these forces change behaviour is known.
It is also observed that if Reynolds number (based on pipe diameter) is less than 21002100 , the flow in a pipe is laminar and if it is greater than 40004000 it is turbulent.

Note:
The number of Reynolds is a dimensionless number that is used in various fluid contexts to distinguish between the turbulent as well as laminar flow of a stream and to anticipate how it will behave.