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Question 5.5: The gas tank contains a 0.6-m depth of gasoline and a 0.2-m ......

The gas tank contains a 0.6-m depth of gasoline and a 0.2-m depth of water as shown in Fig. 5–15. Determine the time needed to drain the water if the drain hole has a diameter of 25 mm. The tank is 1.8 m wide and 3.6 m long. The density of gasoline is ρ_g = 726 kg/m³, and for water, ρ_w = 1000 kg/m³.

fig 5-15
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Fluid Description.   The gasoline is on top of the water because its density is less than that of water. Because the tank is large relative to the drain hole, we will assume steady flow. Also, we will consider the two fluids to be ideal.
Bernoulli Equation.   Here we will select the vertical streamline containing points B and C, Fig. 5–15. At any instant the level of water is h, as measured from the datum, and so the pressure at B is due to the weight of the gasoline above it, that is,
p_B = \gamma _gh_{AB} = (726  kg/m^3)(9.81  m/s^2)(0.6  m) = 4.273(10^3)  N/m^2
To simplify the analysis for using the Bernoulli equation, we will neglect the velocity at B since V_B ≈ 0, and so V_B^2 will be even smaller.
Since C is open to the atmosphere, p_C = 0. Thus,

\frac{p_B}{\gamma _w}  +  \frac{V_B^2}{2g}  +  z_B  =  \frac{p_C}{\gamma _w}  +  \frac{V_C^2}{2g}  +  z_C

 

\frac{4.273 (10^3)  N/m^2}{(1000  kg/m^3)(9.81  m/s^2)}  +  0  +  h  =  0  +  \frac{V_C^2}{2(9.81  m/s^2)}  +  0

 

V_C  =  4.429  \sqrt{h  +  0.4356}        (1)

Continuity Equation.   The continuity of flow at B and C will allow us to relate the actual nonzero V_B to V_C. We will choose a control volume that contains all the water up to the depth h. Since V_B is downward and h is positive upward, then at the top control surface,
V_B = -dh/dt. Thus,

\frac{∂}{∂t}\int_{cv}  \rho  d\sout{V} + \int _{cs} \rho  V_{f/cs} · dA = 0

 

0  –  V_B A_B  +  V_C A_C  =  0

 

0  –  (- \frac{dh}{dt})  [(1.8  m)(3.6  m)]  +  V_C[\pi (0.0125  m)^2]  =  0

 

\frac{dh}{dt}  =  -75.752 (10^{-6})  V_C

Now, using Eq. 1,

\frac{dh}{dt}  =  -75.752 (10^{-6})  (4.429  \sqrt{h  +  0.4356})

or

\frac{dh}{dt}  = -0.3355 (10^{-3}  \sqrt{h  +  0.4356})       (2)

Notice that when h = 0.2 m, V_B = dh/dt = 0.268(10^{-3}) m/s, which is very slow compared to V_C = 3.53 m/s, as determined from Eq. 1, and so indeed we were justified in neglecting V_B^2 in Eq. 1.
If t_d is the time needed to drain the tank, then separating the variables in Eq. 2 and integrating, we get

\int _{0.2  m}^0 \frac{dh}{\sqrt{h  +  0.4356}}  =  -0.3355 (10^{-3})  \int_0^{t_d}   dt

 

(2\sqrt{h  +  0.4356})|_{0.2  m}^0  =  -0.3355 (10^{-3}) t_d

Evaluating the limits, we get

–  0.2745 = – 0.3355 (10^{-3}) t_d

t_d = 818.06 s  =  13.6 min.

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