/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 38 In an unwise effort to remove de... [FREE SOLUTION] | 91Ó°ÊÓ

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In an unwise effort to remove debris, a homeowner directs the nozzle of his backpack blower directly toward the garage door. The nozzle velocity is 130 \(\mathrm{mi} / \mathrm{hr}\) and the flow rate is \(410 \mathrm{ft}^{3} / \mathrm{min} .\) Estimate the force \(F\) exerted by the airflow on the door. The specific weight of air is \(0.0753 \mathrm{lb} / \mathrm{ft}^{3}\).

Short Answer

Expert verified
The force exerted by the airflow on the door is approximately 97.9 pounds.

Step by step solution

01

Convert Velocity to Consistent Units

First, we need to convert the velocity from miles per hour to feet per minute. Since there are 5280 feet in a mile and 60 minutes in an hour, we multiply:\[ 130 \text{ mi/hr } \times \frac{5280 \text{ ft}}{1 \text{ mi}} \times \frac{1 \text{ hr}}{60 \text{ min}} = 11440 \text{ ft/min}. \]
02

Calculate the Mass Flow Rate

Next, we calculate the mass flow rate using the given flow rate and specific weight of air. The mass flow rate \( \dot{m} \) is given by the formula \( \dot{m} = \text{flow rate} \times \text{specific weight} \). So, we have:\[ \dot{m} = 410 \text{ ft}^3/\text{min} \times 0.0753 \text{ lb/ft}^3 = 30.873 \text{ lb/min}. \]
03

Use Momentum Principle to Find Force

Force can be determined using the momentum principle \( F = \dot{m}v \), where \( \dot{m} \) is the mass flow rate and \( v \) is the velocity. Substitute in the values we calculated: \[ F = 30.873 \text{ lb/min} \times 11440 \text{ ft/min} = 352520.4 \text{ lb} \text{ ft/min}^2. \]
04

Convert Force to Pounds

The unit \(\text{lb} \text{ ft/min}^2 \) can be converted into \(\text{lb}\) by using the factor 1 pound in \(1\, \text{g}\) (gravity) which is \(32.2 \text{ ft/s}^2.\) Since there are 60 seconds in a minute, convert the units:\[ 352520.4 \text{ lb } \text{ ft/min}^2 \times \frac{1 \text {min}^2}{3600 \text{ s}^2} = 97.9 \text{ lb}. \]
05

Final Conclusion

Thus, the force exerted by the airflow on the door is approximately 97.9 pounds.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Momentum Principle
The Momentum Principle is a fundamental concept in dynamics that helps us understand how the motion of objects can be influenced by forces. It states that the change in momentum of an object is equal to the impulse applied to it. In mathematical terms, momentum ( p ) is defined as the product of mass ( m ) and velocity ( v ):
  • Momentum: \[ p = m \cdot v \]
  • Change in momentum: \[ \Delta p = F \cdot \Delta t \]
In the context of the exercise, we use the momentum principle to calculate the force ( F ) exerted by the airflow. By knowing the mass flow rate and the velocity of the air, we determine the momentum change, which helps us find the force acting on the door.
The force can be directly calculated with the formula:
  • Force: \[ F = \dot{m} \times v \]
Where \( \dot{m} \) is the mass flow rate, and \( v \) is the velocity of the airflow.
Unit Conversion
Unit conversion is a crucial skill in physics and engineering, ensuring that all measurements are in compatible units for calculations. In this exercise, the velocity of the airflow is initially given in miles per hour (mi/hr). To use this value in our calculations, we need to convert it into feet per minute (ft/min), as the flow rate is given in cubic feet per minute.
Here is the conversion process:
  • Convert miles to feet: \[ 1 \text{ mile} = 5280 \text{ feet} \]
  • Convert hours to minutes: \[ 1 \text{ hour} = 60 \text{ minutes} \]
Using these conversion factors, velocity is calculated as:
  • Velocity: \[ 130 \text{ mi/hr} \times \frac{5280 \text{ ft}}{1 \text{ mi}} \times \frac{1 \text{ hr}}{60 \text{ min}} = 11440 \text{ ft/min} \]
Mass Flow Rate
The mass flow rate is an essential concept in fluid dynamics, quantifying the mass of fluid passing through a section per unit time. It is a vital step when calculating forces involving fluids. In this exercise, we calculate the mass flow rate using the given volumetric flow rate and the specific weight of air.
The formula for mass flow rate (\( \dot{m} \)) is straightforward:
  • Mass flow rate: \[ \dot{m} = \text{Volumetric flow rate} \times \text{Specific weight} \]
Given:
  • Flow rate: 410 \( \text{ft}^3/\text{min} \)
  • Specific weight: 0.0753 \( \text{lb/ft}^3 \)
Hence,
  • \[\dot{m} = 410 \text{ ft}^3/\text{min} \times 0.0753 \text{ lb/ft}^3 = 30.873 \text{ lb/min} \]
Specific Weight of Air
The specific weight of a fluid, such as air, is a significant parameter in many engineering calculations. It is defined as the weight per unit volume, representing how much a particular volume of the fluid weighs. For this exercise, the specific weight of air is given as 0.0753 lb/ft³. This value is crucial when computing the mass flow rate.
Specific weight ( γ ) can be calculated as follows:
  • Specific weight formula: \[ \gamma = \frac{\text{Weight}}{\text{Volume}} \]
In fluid dynamics problems, knowing the specific weight helps in converting volumetric flow rates to mass flow rates since:
  • Mass flow rate: \[ \dot{m} = \text{Flow rate} \times \gamma \]
This parameter allows for more accurate and meaningful calculations, particularly in determining the force exerted by moving air on surfaces like the garage door in the exercise scenario.

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Most popular questions from this chapter

Salt water flows through the fixed 12 -in.-insidediameter pipe at a speed \(v_{0}=4 \mathrm{ft} / \mathrm{sec}\) and enters the \(150^{\circ}\) bend with inside radius of 24 in. The water exits to the atmosphere through the 6 -in.-diameter nozzle \(C\). Determine the shear force \(V\), axial force \(P\), and bending moment \(M\) at flanges \(A\) and \(B\) which result from the flow of the salt water. The gage pressure in the pipe at flange \(A\) is 250 lb/in. \(^{2}\) and the pressure drop between \(A\) and \(B\) due to head loss may be neglected.

A horizontal bar of mass \(m_{1}\) and small diameter is suspended by two wires of length \(l\) from a carriage of mass \(m_{2}\) which is free to roll along the horizontal rails. If the bar and carriage are released from rest with the wires making an angle \(\theta\) with the vertical, determine the velocity \(v_{\text {ble }}\) of the bar relative to the carriage and the velocity \(v_{c}\) of the carriage at the instant when \(\theta=0 .\) Neglect all friction and treat the carriage and the bar as particles in the vertical plane of motion.

A small rocket-propelled vehicle weighs \(125 \mathrm{lb}\), in cluding 20 lb of fuel. Fuel is burned at the constant rate of 2 lb/sec with an exhaust velocity relative to the nozzle of \(400 \mathrm{ft} / \mathrm{sec}\). Upon ignition the vehicle is released from rest on the \(10^{\circ}\) incline. Calculate the maximum velocity \(v\) reached by the vehicle. Neglect all friction.

A model rocket weighs 1.5 lb just before its vertical launch. Its experimental solid-fuel motor carries 0.1 lb of fuel, has an escape velocity of 3000 ft/sec, and burns the fuel for 0.9 sec. Determine the acceleration of the rocket at launch and its burnout velocity. Neglect aerodynamic drag and state any other assumptions.

The 300 -kg and 400 -kg mine cars are rolling in opposite directions along the horizontal track with the respective speeds of \(0.6 \mathrm{m} / \mathrm{s}\) and \(0.3 \mathrm{m} / \mathrm{s}\). Upon impact the cars become coupled together, Just prior to impact, a 100 -kg boulder leaves the delivery chute with a velocity of \(1.2 \mathrm{m} / \mathrm{s}\) in the direction shown and lands in the 300 -kg car. Calculate the velocity \(v\) of the system after the boulder has come to rest relative to the car. Would the final velocity be the same if the cars were coupled before the boulder dropped?

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