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Svetlanka [38]
3 years ago
8

. A long 10-cm-diameter steam pipe whose external surface temperature is 110oC passes through some open area that is not protect

ed against the winds. Determine the rate of heat loss from the pipe per unit of its length when the air is at 1 atm pressure and 10oC and the wind is blowing across the pipe at a velocity of 8 m/s. Use the following relation to calculate the Nusselt number.
Physics
2 answers:
Nata [24]3 years ago
8 0

Answer:

Nu = 30.311

Explanation:

Let consider that pipe is a horizontal cylinder. The Nusselt number is equal to:

Nu = \left\{0.6+\frac{0.387\cdot Ra_{D}^{\frac{1}{6} }}{[1+\left(\frac{0.559}{Pr}  \right)^{\frac{9}{16}} ]^{\frac{8}{27} }}  \right\}^{2}, for Ra_{D} \le 10^{12}.

Where Ra_{D} is the Rayleigh number associated with the cylinder.

The Rayleigh number is:

Ra_{D} = \frac{g\cdot \beta\cdot (T_{pipe}-T_{air})\cdot D^{3}}{\nu^{2}}\cdot Pr

By assuming that air behaves ideally, the coefficient of volume expansion is:

\beta = \frac{1}{T}

\beta = \frac{1}{283.15\,K}

\beta = 3.532\times 10^{-3}\,\frac{1}{K}

The cinematic and dynamic viscosities, thermal conductivity and isobaric specific heat of air at 10 °C and 1 atm are:

\nu = 1.426\times 10^{-5}\,\frac{m^{2}}{s}

\mu = 1.778\times 10^{-5}\,\frac{kg}{m\cdot s}

k = 0.02439\,\frac{W}{m\cdot ^{\textdegree}C}

c_{p} = 1006\,\frac{J}{kg\cdot ^{\textdegree}C}

The Prandtl number is:

Pr = \frac{\mu\cdot c_{p}}{k}

Pr = \frac{(1.778\times 10^{-5}\,\frac{kg}{m\cdot s} )\cdot (1006\,\frac{J}{kg\cdot ^{\textdegree}C} )}{0.02439\,\frac{W}{m\cdot ^{\textdegree}C} }

Pr = 0.733

Likewise, the Rayleigh number is:

Ra_{D} = \frac{(9.807\,\frac{m}{s^{2}} )\cdot (3.532\times 10^{-3}\,\frac{1}{K} )\cdot (110^{\textdegree}C-10^{\textdegree}C)\cdot (0.1\,m)^{3}}{(1.426\times 10^{-5}\,\frac{m^{2}}{s})^{2} }\cdot (0.733)

Ra_{D} = 12.486\times 10^{6}

Finally, the Nusselt number is:

Nu = \left\{0.6+\frac{0.387\cdot (12.486\times 10^{6})^{\frac{1}{6} }}{\left[1 + \left(\frac{0.559}{0.733}\right)^{\frac{9}{16} }\right]^{\frac{8}{27} }}  \right\}^{2}

Nu = 30.311

vlada-n [284]3 years ago
5 0

Answer:

The Nusselt number = 124

Explanation:

Our assumption is that air is an ideal gas and that the radiation effect is negligible

Surface temperature, T_{s} = 110^{0} C

T_{\infty} = 10^{0} C

Velocity, v = 8 m/s

The film temperature can be calculated as, T_{f} = \frac{T_{s} + T_{\infty} }{2}

T_{f} = \frac{110 +10 }{2} \\T_{f} = 60^{0} C

At the film temperature, T_{f} = 60^{0} C and  1 atm pressure, air has the following properties:

K = 0.02808 W/m-k

P_{r} = 0.7202

Reynold number, Re = \frac{vD}{V}

D = 10 cm = 0.1 m

V = 1.896 * 10⁻⁵ m²/s

Re = \frac{0.1 * 8}{1.896 * 10^{-5} }

Re = 4.2194 * 10⁴

The Nusselt number will be calculated using the relation:

Nu = 0.3 + \frac{0.62 Re^{1/2} Pr^{1/3} }{[1 +( 0.41 Pr)^{2/3}] ^{1/4} } + [1 + (\frac{Re}{282000} )^{5/8} ]^{4/5}

Substituting Re = 4.2194 * 10⁴ and P_{r} = 0.7202 into the equation above

the Nusselt number, Nu = 124

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Explanation:

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       K_{trans} = \frac{1}{2}* M* v_{cm} ^{2}  (1)

  • The rotational part can be expressed as follows:

       K_{rot} = \frac{1}{2}* I* \omega ^{2}  (2)

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       v = \omega * R (3)

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       K_{rot} = \frac{1}{2}* \frac{1}{2} M*R^{2} * \frac{v_{cmc} ^{2}}{R^{2}} = \frac{1}{4}* M* v_{cmc}^{2}  (5)

  • Adding (5) and (1), we get the total kinetic energy for the solid cylinder, as follows:

       K_{cyl} = \frac{1}{2}* M* v_{cmc} ^{2}  +\frac{1}{4}* M* v_{cmc}^{2}  =  \frac{3}{4}* M* v_{cmc} ^{2} (6)

  • Repeating the same steps for the spherical shell:

        I_{sph} = \frac{2}{3} * M* R^{2} (7)  

       K_{rot} = \frac{1}{2}* \frac{2}{3} M*R^{2} * \frac{v_{cms} ^{2}}{R^{2}} = \frac{1}{3}* M* v_{cms}^{2}  (8)

      K_{sph} = \frac{1}{2}* M* v_{cms} ^{2}  +\frac{1}{3}* M* v_{cms}^{2}  =  \frac{5}{6}* M* v_{cms} ^{2} (9)

  • Since we know that both masses are equal each other, we can simplify (6) and (9), cancelling both masses out.
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       \frac{v_{cmc}}{v_{cms}} =\sqrt{\frac{10}{9} } = 1.05 (10)

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The rifle barrel must be pointed at a height of 4.45cm above the target so that the bullet hits dead center.

Explanation:

First, we need to sketch the situation so we can have a better idea of what the problem looks like (Refer to uploaded picture).

So as you may see in the drawing, when pointing the rifle to the target, we can see it as a triangle, but in reality, the bullet will have a parabolic trajectory. Both points of view will help us determine what the height must be. In order to find it, we need to first determine at what angle the bullet should be shot. In order to do so we can use the range formula, which looks like this:

R=\frac{v^{2}sin(2\theta)}{g}

Where R is the range of the bullet (this is how far it goes before it has the

same height it was shot from), v is the original speed of the bullet, θ is the angle at which the bullet is shot and g is the acceleration of gravity.

We can solve this equation for theta, so we get:

gR=v^{2}sin(2\theta)

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so now we can substitute the given data:

\theta=\frac{sin^{-1}(\frac{(9.8m/s^{2})(45.5m)}{(477m/s)^{2}})}{2}

so we get:

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once we get the angle, we can look at the triangle diagram. From the drawing we can see that we can use the tan function to find the height:

tan \theta = \frac{h}{45.5m}

so we can solve this for h, so we get:

h=45.5m*tan(0.05614^{o})

which yields:

h=0.0445m

or

h=4.45cm

5 0
3 years ago
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