/*! 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 13 A helicopter of mass \(m\) is ta... [FREE SOLUTION] | 91Ó°ÊÓ

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A helicopter of mass \(m\) is taking off vertically. The only forces acting on it are the earth's gravitational force and the force, \(F_{a i r}\), of the air pushing up on the propeller blades. (a) If the helicopter lifts off at \(t=0\), what is its vertical speed at time \(t\) ? (b) Check that the units of your answer to part a make sense. (c) Discuss how your answer to part a depends on all three variables, and show that it makes sense. That is, for each variable, discuss what would happen to the result if you changed it while keeping the other two variables constant. Would a bigger value give a smaller result, or a bigger result? Once you've figured out this mathematical relationship, show that it makes sense physically. (d) Plug numbers into your equation from part a, using \(m=2300 \mathrm{~kg}, F_{a i r}=27000 \mathrm{~N}\), and \(t=4.0 \mathrm{~s}\). (answer check available at lightandmatter.com)

Short Answer

Expert verified
The helicopter's speed after 4 seconds is 7.74 m/s.

Step by step solution

01

Understanding the forces

The helicopter is subject to two forces: the gravitational force and the air force on the propeller blades. The gravitational force is given by \( F_{ ext{gravity}} = mg \), where \( g \approx 9.8 \, \text{m/s}^2 \) is the acceleration due to gravity. The lifting force provided by the air is \( F_{\text{air}} \). According to Newton's second law, \( F_{\text{net}} = m a \), where \( F_{\text{net}} = F_{\text{air}} - F_{\text{gravity}} \).
02

Calculating acceleration

Using Newton's second law, we set up the equation for net force: \[ F_{\text{air}} - mg = ma \]. Solving for acceleration \( a \), we get: \[ a = \frac{F_{\text{air}} - mg}{m} \].
03

Finding vertical speed

The initial vertical speed \( v_i \) at \( t = 0 \) is zero because the helicopter is taking off. To find the speed after time \( t \), use the kinematic equation: \[ v = v_i + at \]. Substituting \( v_i = 0 \) and the expression for \( a \), we have: \[ v(t) = \frac{F_{\text{air}} - mg}{m} \times t \].
04

Checking units

Check that units match by substituting the given units into the equation. The units for force are \( \text{N} = \text{kg} \, \text{m/s}^2 \), and the units for mass \( m \) are \( \text{kg} \). Therefore, \[ \text{Units of } \left(\frac{\text{N}}{\text{kg}}\right) \text{ are } \text{m/s}^2 \]. Multiply by \( \text{s} \) to get units of velocity, \( \text{m/s} \), which confirms the units of the answer are correct.
05

Analyzing dependency on variables

The result \( v(t) = \left(\frac{F_{\text{air}} - mg}{m}\right) t \) depends on \( F_{\text{air}} \), \( m \), and \( t \):- Increasing \( F_{\text{air}} \) increases \( v(t) \) since \( a \) becomes larger.- Increasing \( m \) decreases \( v(t) \) because the same force results in a smaller acceleration.- \( v(t) \) is directly proportional to \( t \); longer time results in higher speed.These relationships make sense physically: more lifting force leads to faster acceleration, a larger mass requires more force to achieve the same speed, and speed builds over time.
06

Plugging in numerical values

Substitute \( m = 2300 \, \text{kg} \), \( F_{\text{air}} = 27000 \, \text{N} \), and \( t = 4.0 \, \text{s} \) into the equation:\[ v(t) = \left(\frac{27000 \, \text{N} - 2300 \, \text{kg} \times 9.8 \, \text{m/s}^2}{2300 \, \text{kg}}\right) \times 4.0 \, \text{s} \].Calculate the specific values to find the result.
07

Calculations

First, calculate the weight of the helicopter: \[ mg = 2300 \, \text{kg} \times 9.8 \, \text{m/s}^2 = 22540 \, \text{N} \].Subtract this from the lifting force:\[ F_{\text{air}} - mg = 27000 \, \text{N} - 22540 \, \text{N} = 4450 \, \text{N} \].Calculate acceleration:\[ a = \frac{4450 \, \text{N}}{2300 \, \text{kg}} = 1.935 \, \text{m/s}^2 \].Finally, the speed after 4 seconds:\[ v(t) = 1.935 \, \text{m/s}^2 \times 4.0 \, \text{s} = 7.74 \, \text{m/s} \].

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Key Concepts

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

Newton's Second Law
In the realm of physics, Newton's Second Law of Motion is a cornerstone. It helps us understand the relationship between the forces acting upon an object and its acceleration. According to this law, the net force acting on an object is equal to the mass of that object multiplied by its acceleration, expressed as \( F_{\text{net}} = ma \). In simpler terms, if you know two of these quantities, you can solve for the third.
For a helicopter taking off, the two primary forces at play are gravity pulling it down, and the air force from the propellers pushing it up. The net force here is the upward force minus the gravitational force, or the difference between the air force \( F_{\text{air}} \) and the gravitational force \( mg \).
Using Newton’s Second Law, you can determine the net force and in turn, calculate the helicopter's acceleration. It's a powerful way to see how different forces impact the motion of objects.
Acceleration Calculation
Once you understand the forces, the next step is to calculate acceleration. Acceleration measures how quickly an object speeds up or slows down. Using Newton’s Second Law, you can rearrange the formula \( F_{\text{net}} = ma \) to solve for acceleration, giving you \( a = \frac{F_{\text{net}}}{m} \). For the helicopter, this becomes \( a = \frac{F_{\text{air}} - mg}{m} \).
This equation tells us that:
  • Increasing the force from the air \( F_{\text{air}} \) increases the acceleration, resulting in faster lift-off.
  • Increasing the helicopter's mass \( m \) without increasing the force reduces the acceleration, making lift-off slower.
If you know the net force and the helicopter's mass, you can easily compute its acceleration. Keep in mind that this acceleration defines the rate of change of speed over time.
Kinematic Equations
Kinematic equations are vital for solving motion problems with constant acceleration. For the helicopter, we use the kinematic equation \( v = v_i + at \) to find its vertical speed at a given time \( t \). Here, \( v_i \) is the initial velocity, which is 0 since the helicopter starts from rest.
Substituting the acceleration equation we derived earlier, the formula becomes \[ v(t) = \left(\frac{F_{\text{air}} - mg}{m}\right) t \].
These equations allow us to predict the helicopter's speed at any time after take-off, assuming a constant force from the air and gravitational forces. Kinematic equations make it possible to understand how variables like time \( t \), force \( F_{\text{air}} \), and mass \( m \) interact and affect the helicopter's motion:
  • Longer times \( t \) result in higher speeds, as the helicopter continually accelerates.
  • More force and less mass mean greater acceleration and thus faster speeds.
Kinematic equations provide a clear picture of the speeds and positions, showing the progress of the helicopter during its ascent.

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Most popular questions from this chapter

Someone tells you she knows of a certain type of Central American earthworm whose skin, when rubbed on polished diamond, has \(\mu_{k}>\mu_{s}\). Why is this not just empirically unlikely but logically suspect?

If you walk \(35 \mathrm{~km}\) at an angle \(25^{\circ}\) counterclockwise from east, and then \(22 \mathrm{~km}\) at \(230^{\circ}\) counterclockwise from east, find the distance and direction from your starting point to your destination. (answer check available at lightandmatter.com)

A car accelerates from rest. At low speeds, its acceleration is limited by static friction, so that if we press too hard on the gas, we will "burn rubber" (or, for many newer cars, a computerized traction-control system will override the gas pedal). At higher speeds, the limit on acceleration comes from the power of the engine, which puts a limit on how fast kinetic energy can be developed. (a) Show that if a force \(F\) is applied to an object moving at speed \(v\), the power required is given by \(P=v F\). (b) Find the speed \(v\) at which we cross over from the first regime described above to the second. At speeds higher than this, the engine does not have enough power to burn rubber. Express your result in terms of the car's power \(P\), its mass \(m\), the coefficient of static friction \(\mu_{s}\), and \(g\).(answer check available at lightandmatter.com) (c) Show that your answer to part b has units that make sense. (d) Show that the dependence of your answer on each of the four variables makes sense physically. (e) The 2010 Maserati Gran Turismo Convertible has a maximum power of \(3.23 \times 10^{5} \mathrm{~W}\) (433 horsepower) and a mass (including a 50 -kg driver) of \(2.03 \times 10^{3} \mathrm{~kg}\). (This power is the maximum the engine can supply at its optimum frequency of 7600 r.p.m. Presumably the automatic transmission is designed so a gear is available in which the engine will be running at very nearly this frequency when the car is at moving at \(v .\).) Rubber on asphalt has \(\mu_{s} \approx 0.9 .\) Find \(v\) for this car. Answer: \(18 \mathrm{~m} / \mathrm{s}\), or about 40 miles per hour. (f) Our analysis has neglected air friction, which can probably be approximated as a force proportional to \(v^{2}\). The existence of this force is the reason that the car has a maximum speed, which is 176 miles per hour. To get a feeling for how good an approximation it is to ignore air friction, find what fraction of the engine's maximum power is being used to overcome air resistance when the car is moving at the speed \(v\) found in part e.

(solution in the pdf version of the book) When the contents of a refrigerator cool down, the changed molecular speeds imply changes in both momentum and energy. Why, then, does a fridge transfer power through its radiator coils, but not force?

Mountain climbers with masses \(m\) and \(M\) are roped together while crossing a horizontal glacier when a vertical crevasse opens up under the climber with mass \(M\). The climber with mass \(m\) drops down on the snow and tries to stop by digging into the snow with the pick of an ice ax. Alas, this story does not have a happy ending, because this doesn't provide enough friction to stop. Both \(m\) and \(M\) continue accelerating, with \(M\) dropping down into the crevasse and \(m\) being dragged across the snow, slowed only by the kinetic friction with coefficient \(\mu_{k}\) acting between the ax and the snow. There is no significant friction between the rope and the lip of the crevasse. (a) Find the acceleration \(a\).(answer check available at lightandmatter.com) (b) Check the units of your result. (c) Check the dependence of your equation on the variables. That means that for each variable, you should determine what its effect on \(a\) should be physically, and then what your answer from part a says its effect would be mathematically.

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