(II)Estimate the air pressure inside a category 5 hurricane, where the wind speed is 300 km/h (Fig. 10-52).

Short Answer

Expert verified

The air pressure inside a category 5 hurricane is \(96.78\;{\rm{kPa}}\).

Step by step solution

01

Understanding the Bernoulli’s equation

The air pressure inside a hurricane can be estimated by utilizing the reduced form of Bernoulli’s equation.

02

Given data

The wind speed inside the hurricane is \({v_1} = 300\;{\rm{km/h}}\).

The standard value for the density of air is \(\rho = 1.3\;{\rm{kg/}}{{\rm{m}}^3}\), and the pressure outside the hurricane is equal to atmospheric pressure \({P_1} = {P_{atm}} = 101.3 \times {10^3}\;{\rm{Pa}}\).

03

Evaluating the air pressure inside the hurricane

The air pressure inside a hurricane is calculated below:

\(\begin{array}{c}{P_1} - {P_2} = \frac{1}{2}\rho \left( {{{\left( {{v_2}} \right)}^2} - {{\left( {{v_1}} \right)}^2}} \right)\\{P_1} - {P_2} = \frac{1}{2}\rho \left( {{{\left( 0 \right)}^2} - {{\left( {{v_1}} \right)}^2}} \right)\\{P_1} - {P_2} = \frac{1}{2}\rho {\left( {{v_1}} \right)^2}\\{P_2} = {P_1} - \frac{1}{2}\rho {\left( {{v_1}} \right)^2}\end{array}\)

Here, \({v_2}\) is the wind speed outside the hurricane.

Substitute the values in the above equation.

\(\begin{array}{c} = 101.3 \times {10^3}\;{\rm{Pa}} - \left( {\frac{1}{2}\left( {1.3\;{\rm{kg/}}{{\rm{m}}^3}} \right){{\left( {300\;{\rm{km/h}} \times \frac{{1000\;{\rm{m}}}}{{1\;{\rm{km}}}} \times \frac{{1\;{\rm{h}}}}{{3600\;{\rm{s}}}}} \right)}^2}} \right)\\ = 96786.47\;{\rm{Pa}} \times \left( {\frac{{1\;{\rm{kPa}}}}{{1000\;{\rm{Pa}}}}} \right)\\ = 96.78\;{\rm{kPa}}\end{array}\)

Hence, the air pressure inside a hurricane is \(96.78\;{\rm{kPa}}\).

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Most popular questions from this chapter

(I)Calculate the average speed of blood flow in the major arteries of the body, which have a total cross-sectional area of about \(2.0\;{\rm{c}}{{\rm{m}}^2}\). Use the data of Example 10–12.

(II) Poiseuille’s equation does not hold if the flow velocity is high enough that turbulence sets in. The onset of turbulence occurs when the Reynolds number, \(Re\) , exceeds approximately 2000. \(Re\) is defined as

\({\mathop{\rm Re}\nolimits} = \frac{{2\overline v r\rho }}{\eta }\)

where \(\overline v \) is the average speed of the fluid, \(\rho \) is its density, \(\eta \) is its viscosity, and \(r\) is the radius of the tube in which the fluid is flowing. (a) Determine if blood flow through the aorta is laminar or turbulent when the average speed of blood in the aorta \(\left( {{\bf{r = 0}}{\bf{.80}}\;{\bf{cm}}} \right)\) during the resting part of the heart’s cycle is about \({\bf{35}}\;{\bf{cm/s}}\). (b) During exercise, the blood-flow speed approximately doubles. Calculate the Reynolds number in this case, and determine if the flow is laminar or turbulent.

(I) Estimate the pressure exerted on a floor by (a) a one-pointed heel of area = 0.45 cm2, and (b) one wide heel of area 16 cm2, Fig. 10–48. The person wearing the shoes has a mass of 56 kg.


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