/*! 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 28 A model of a helicopter rotor ha... [FREE SOLUTION] | 91Ó°ÊÓ

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A model of a helicopter rotor has four blades, each \(3.40 \mathrm{~m}\) long from the central shaft to the blade tip. The model is rotated in a wind tunnel at 550 rev \(/\) min. (a) What is the linear speed of the blade tip, in \(\mathrm{m} / \mathrm{s} ?\) (b) What is the radial acceleration of the blade tip expressed as a multiple of \(g ?\)

Short Answer

Expert verified
The linear speed of the blade tip is 196 m/s, and the radial acceleration of the blade tip is 1150 times the acceleration due to gravity.

Step by step solution

01

Converting Rotational Speed

First, the rotational speed (550 revolutions/minute) has to be converted to the standard scientific units: revolutions per second (rev/s). \[550 \text{ rev/min} \times \frac{1 \text{ min}}{60 \text{ s}} = 9.17 \text{ rev/s}\] Now the rotation speed is in a form we can use with standard physics formulas.
02

Calculate Linear Speed

The linear speed (v) of the tip of a blade can be calculated using the formula: \[v = r\omega\] where r is the length of the blade (3.4 m) and \(\omega\) is the rotational speed in radians per second. But before we get to that, remember to convert the given rotational speed to radians per second by multiplying by \(2\pi\): \[9.17 \text{ rev/s} \times 2\pi \text{ rad/rev} = 57.6 \text{ rad/s}\] Now we can calculate the linear speed: \[v = 3.4 \text{ m} \times 57.6 \text{ rad/s} = 196 \text{ m/s}\]
03

Calculate Radial Acceleration

Now we can calculate the radial acceleration, using the formula: \[a = \frac{v^2}{r}\] Substituting the values gives: \[a = \frac{(196 \text{ m/s})^2}{3.4 \text{ m}} = 11300 \text{ m/s}^2\]
04

Express Radial Acceleration as Multiple of g

To find the radial acceleration as a multiple of gravity (g), we divide the radial acceleration by the acceleration due to gravity (approximately 9.8 m/s²): \[a_g = \frac{11300 \text{ m/s}^2}{9.8 \text{ m/s}^2} = 1150g\] This means that the radial acceleration of the tip of the blade is 1150 times the acceleration due to gravity.

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Key Concepts

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

Rotational Kinematics
Rotational kinematics is all about understanding motion in a circular path. This involves the study of how objects rotate around an axis. In this problem, a helicopter rotor spins around a central shaft, covering circular motion. The rotor spins at a rate of 550 revolutions per minute.
This rotational speed needs to be converted into a form that we can use with physics formulas, specifically revolutions per second. To change from revolutions per minute to revolutions per second, divide by 60. This step is key because it brings the units to a manageable and standard form. Always ensure your units align correctly in physics to simplify solving the problem.
  • Convert 550 revolutions per minute to 9.17 revolutions per second by dividing by 60.
Understanding these basic principles of rotational kinematics allows you to calculate speeds and accelerations in rotating systems, setting a foundation for more complex dynamics calculations.
Linear Speed Calculation
Linear speed is the speed at which a point travels along its path. For a rotating object like a helicopter blade, linear speed can be calculated using the relationship between radial distance (the length of the blade) and angular speed (in radians per second). The formula to find linear speed (v) is
  • \(v = r\omega\)
where \(r\) is the radius (length of the blade), and \(\omega\) is the angular velocity in radians per second.
To convert revolutions per second to radians per second, multiply by \(2\pi\), which gives the conversion we need as a circle has \(2\pi\) radians. This conversion helps you move from a more abstract rotational speed to a tangible rate of motion.
Once you have that angular speed in radians per second, plug it into the linear speed formula. Computing this step might involve multiple operations, but the key is understanding how linear speed connects directly to how fast the whole system is spinning.
Radial Acceleration
Radial acceleration, also known as centripetal acceleration, refers to the acceleration an object experiences towards the center of its circular path. It provides the necessary force to keep the object moving in that circle. For the helicopter blade, the radial acceleration can be calculated with:
  • \(a = \frac{v^2}{r}\)
where \(v\) is the calculated linear speed, and \(r\) is the radial distance (length of the blade). This formula shows how radial acceleration increases rapidly with speed or as the radius decreases.
Calculating a high radial acceleration implies significant forces acting on the blades, highlighting why engineering design needs exact calculations in real-world scenarios like helicopters to avoid structural failures.
For example, in this exercise, the calculations show extremely high radial accelerations, demonstrating how critical it is to understand the forces involved in circular motion.
Conversion of Units
Converting units is essential in physics as it ensures calculations align with the universally accepted systems of measurements. In our problem, several conversions are crucial:
  • Revolutions per minute to revolutions per second (by dividing by 60).
  • Subsequently, converting revolutions per second to radians per second (by multiplying by \(2\pi\)).
Without these conversions, you can't use standard equations to calculate linear speed and radial acceleration accurately. Pay attention to these conversions, as omitting them or making mistakes here can lead to incorrect solutions.
Similarly, when expressing forces or accelerations concerning gravity, ensure the units are consistent. Dividing radial acceleration by gravitational acceleration lets you understand how these forces stack up against the force we experience daily due to gravity. This practice provides a relatable context to the otherwise abstract calculations, offering a clearer understanding of their real-life significance.

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Most popular questions from this chapter

A rookie quarterback throws a football with an initial upward velocity component of \(12.0 \mathrm{~m} / \mathrm{s}\) and a horizontal velocity component of \(20.0 \mathrm{~m} / \mathrm{s}\). Ignore air resistance. (a) How much time is required for the football to reach the highest point of the trajectory? (b) How high is this point? (c) How much time (after it is thrown) is required for the football to return to its original level? How does this compare with the time calculated in part (a) (d) How far has the football traveled horizontally during this time? (e) Draw \(x-t, y-t, v_{x}-t,\) and \(v_{y}-t\) graphs for the motion.

An airplane pilot wishes to fly due west. A wind of \(80.0 \mathrm{~km} / \mathrm{h}\) (about \(50 \mathrm{mi} / \mathrm{h}\) ) is blowing toward the south. (a) If the airspeed of the plane (its speed in still air) is \(320.0 \mathrm{~km} / \mathrm{h}\) (about \(200 \mathrm{mi} / \mathrm{h}),\) in which direction should the pilot head? (b) What is the speed of the plane over the ground? Draw a vector diagram.

The earth has a radius of \(6380 \mathrm{~km}\) and turns around once on its axis in \(24 \mathrm{~h}\). (a) What is the radial acceleration of an object at the earth's equator? Give your answer in \(\mathrm{m} / \mathrm{s}^{2}\) and as a fraction of \(g .\) (b) If \(a_{\mathrm{rad}}\) at the equator is greater than \(g\), objects will fly off the earth's surface and into space. (We'll see the reason for this in Chapter 5.) What would the period of the earth's rotation have to be for this to occur?

A baseball thrown at an angle of \(60.0^{\circ}\) above the horizontal strikes a building \(18.0 \mathrm{~m}\) away at a point \(8.00 \mathrm{~m}\) above the point from which it is thrown. Ignore air resistance. (a) Find the magnitude of the ball's initial velocity (the velocity with which the ball is thrown). (b) Find the magnitude and direction of the velocity of the ball just before it strikes the building.

A snowball rolls off a barn roof that slopes downward at an angle of \(40^{\circ}\) (Fig. \(\mathbf{P 3 . 6 1}\) ). The edge of the roof is \(14.0 \mathrm{~m}\) above the ground, and the snowball has a speed of \(7.00 \mathrm{~m} / \mathrm{s}\) as it rolls off the roof. Ignore air resistance. (a) How far from the edge of the barn does the snowball strike the ground if it doesn't strike anything else while falling? (b) Draw \(x-t, y-t, v_{x}-t,\) and \(v_{y}-t\) graphs for the motion in part (a). (c) A man \(1.9 \mathrm{~m}\) tall is standing \(4.0 \mathrm{~m}\) from the edge of the barn. Will the snowball hit him?

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