/*! 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

Crickets Chirpy and Milada jump from the top of a vertical cliff. Chirpy drops downward and reaches the ground in \(2.70 \mathrm{~s},\) while Milada jumps horizontally with an initial speed of \(95.0 \mathrm{~cm} / \mathrm{s}\). How far from the base of the cliff will Milada hit the ground? Ignore air resistance.

A roller coaster car moves in a vertical circle of radius \(R\). At the top of the circle the car has speed \(v_{1}\), and at the bottom of the circle it has speed \(v_{2},\) where \(v_{2}>v_{1} .\) (a) When the car is at the top of its circular path, what is the direction of its radial acceleration, \(a_{\mathrm{rad}, \text { top }} ?\) (b) When the car is at the bottom of its circular path, what is the direction of its radial acceleration, \(a_{\mathrm{rad}, \text { bottom }} ?\) (c) In terms of \(v_{1}\) and \(v_{2}\), what is the ratio \(a_{\text {rad, bottom }} / a_{\text {rad, top }} ?\)

Firefighters use a high-pressure hose to shoot a stream of water at a burning building. The water has a speed of \(25.0 \mathrm{~m} / \mathrm{s}\) as it leaves the end of the hose and then exhibits projectile motion. The firefighters adjust the angle of elevation \(\alpha\) of the hose until the water takes \(3.00 \mathrm{~s}\) to reach a building \(45.0 \mathrm{~m}\) away. Ignore air resistance; assume that the end of the hose is at ground level. (a) Find \(\alpha\). (b) Find the speed and acceleration of the water at the highest point in its trajectory. (c) How high above the ground does the water strike the building, and how fast is it moving just before it hits the building?

The froghopper, Philaenus spumarius, holds the world record for insect jumps. When leaping at an angle of \(58.0^{\circ}\) above the horizontal, some of the tiny critters have reached a maximum height of \(58.7 \mathrm{~cm}\) above the level ground. (See Nature, Vol. 424, July \(31,2003,\) p. 509.) Neglect air resistance in answering the following. (a) What was the takeoff speed for such a leap? (b) What horizontal distance did the froghopper cover for this world- record leap?

Two students are canoeing on a river. While heading upstream, they accidentally drop an empty bottle overboard. They then continue paddling for 60 minutes, reaching a point \(2.0 \mathrm{~km}\) farther upstream. At this point they realize that the bottle is missing and, driven by ecological awareness, they turn around and head downstream. They catch up with and retrieve the bottle (which has been moving along with the current) \(5.0 \mathrm{~km}\) downstream from the turnaround point. (a) Assuming a constant paddling effort throughout, how fast is the river flowing? (b) What would the canoe speed in a still lake be for the same paddling effort?

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