/*! 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 55 A ski tow operates on a \(15.0^{... [FREE SOLUTION] | 91Ó°ÊÓ

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A ski tow operates on a \(15.0^{\circ}\) slope of length \(300 \mathrm{~m}\). The rope moves at \(12.0 \mathrm{~km} / \mathrm{h}\) and provides power for 50 riders at one time, with an average mass per rider of \(70.0 \mathrm{~kg}\). Estimate the power required to operate the tow.

Short Answer

Expert verified
The power required to operate the tow is approximately 8.91 MW.

Step by step solution

01

Calculate Force

Firstly, the force exerted by all riders has to be calculated. This is simply the product of the total mass of the riders, which is difference in elevation (height) and gravitational acceleration (\(9.8 \mathrm{~m/s^2}\)). Total mass is \(50 \times 70 \, \mathrm{kg} = 3500\, \mathrm{kg}\). The height of the slope is calculated as \(300\, \mathrm{m} \times \sin{15^{\circ}} \approx 77.94\, \mathrm{m}\). So, the force is thus \(3500\, \mathrm{kg} \times 9.8\, \mathrm{m/s^2} \times 77.94\, \mathrm{m} \approx 2.672 \times 10^6\, \mathrm{N}\).
02

Calculate Time

The time taken to transport the 50 riders up the slope is obtained from the definition of speed as \(v = \frac{d}{t}\). Rearranging for \(t\) gives \(t = \frac{d}{v}\). Using \(d = 300\, \mathrm{m}\) and speed \(v = 12 \, \mathrm{km/h} = 3.33\, \mathrm{m/s}\), we find the time to be \(t = \frac{300\, \mathrm{m}}{3.33\, \mathrm{m/s}} \approx 90\, \mathrm{s}\).
03

Calculate Power

Finally, plug the values of force and time into the equation of power \(P = \frac{W}{t}\). Since work \(W\) is force times distance (\(300\, \mathrm{m}\)), the required power is \(P = \frac{2.672 \times 10^6\, \mathrm{N} \times 300\, \mathrm{m}}{90\, \mathrm{s}} \approx 8.91 \times 10^6\, \mathrm{W}\) or \(8.91\, \mathrm{MW}\).

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Key Concepts

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

Calculating Force
Grasping the concept of force is crucial when studying physics, especially in problems involving motion and mechanics.
In the given problem, we're looking at a scenario with skiers being pulled up a slope. To understand how much power the ski tow needs, we have to first calculate the force required to pull the riders. Force is a vector quantity that is fundamental to mechanics and is defined by Sir Isaac Newton's Second Law of Motion, which states that the force applied to an object is equal to the mass of that object multiplied by its acceleration (\( F = m \times a \)).

For cases concerning gravity, the acceleration is that of gravity, denoted as 'g', which on Earth is approximately \( 9.8 \text{ m/s}^2 \) at sea level.
  • First, determine the total mass of the riders by multiplying the average rider mass by the number of riders (\( 50 \times 70\text{ kg} = 3500\text{ kg} \)).
  • Next, you calculate the force exerted by this mass along the slope by taking into account the gravitational pull and the height of the slope which correlates to the sin component of the angle due to the incline (\( g \times m \times \text{height} \)).
By understanding these fundamentals, calculating force becomes not just a process of plugging numbers but also an application of fundamental physical laws.
Gravitational Acceleration
Gravitational acceleration is central to many physics problems, especially when analyzing movements within the Earth's gravitational field.
Whether it's a ball thrown upwards or a ski tow moving riders along a slope, the constant acceleration of gravity impacts these motions. In our textbook problem, gravity is the force pulling the skiers down the slope, countered by the ski tow's force pulling them up.

Gravitational acceleration (\( g \)) is approximately \( 9.8 \text{ m/s}^2 \) close to the Earth's surface, but it decreases with altitude. It's important to note that gravitational acceleration is a vector, which means it has both magnitude and direction - toward the center of the Earth. When dealing with inclined planes, like our ski slope,

How do we account for gravitational acceleration?

  • Since we're working on a slope, only the component of gravitational force parallel to the slope is relevant for calculating the force needed by the ski tow. This is where trigonometry comes in: you use the angle of the slope (in this case, 15 degrees) to determine the effective component of gravitational force.
Understanding gravitational acceleration not only helps in calculating forces but also informs concepts like potential energy, orbits, and the behavior of pendulums.
Mechanical Power
The key to understanding mechanical power lies in recognizing its definition: it's the rate of doing work or the rate of energy transfer in mechanical processes.
In simpler terms, mechanical power quantifies how quickly work can be done or how fast energy is used or produced by a mechanical system. In our exercise, this relates to the ski tow's capability to move skiers up the hill. The power required for this action can be substantial due to the forces involved.

Power (\( P \)) is mathematically defined as work (\( W \)) done over time (\( t \)), expressed by the equation \( P = \frac{W}{t} \). Work, in turn, is defined as the force applied over a distance (\( W = F \times d \)).
  • To find the power required for the ski tow, we find the work done by multiplying the force required to pull the skiers (calculated in the force section) by the distance of the slope.
  • Then, we divide this work by the time it takes for the ski tow to move the skiers the length of the slope (calculated using the tow's speed).
By understanding these relationships, one can determine the power output necessary for various mechanical tasks, including lifting objects against gravity, which directly applies to the ski tow scenario.

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Most popular questions from this chapter

Use the work-energy theorem to solve each of these problems. You can use Newton's laws to check your answers. (a) A skier moving at \(5.00 \mathrm{~m} / \mathrm{s}\) encounters a long, rough horizontal patch of snow having a coefficient of kinetic friction of 0.220 with her skis. How far does she travel on this patch before stopping? (b) Suppose the rough patch in part (a) was only \(2.90 \mathrm{~m}\) long. How fast would the skier be moving when she reached the end of the patch? (c) At the base of a frictionless icy hill that rises at \(25.0^{\circ}\) above the horizontal, a toboggan has a speed of \(12.0 \mathrm{~m} / \mathrm{s}\) toward the hill. How high vertically above the base will it go before stopping?

A small block with a mass of \(0.0600 \mathrm{~kg}\) is attached to a cord passing through a hole in a frictionless, horizontal surface (Fig. \(\mathrm{P} 6.71\) ). The block is originally revolving at a distance of \(0.40 \mathrm{~m}\) from the hole with a speed of \(0.70 \mathrm{~m} / \mathrm{s}\) The cord is then pulled from below, shortening the radius of the circle in which the block revolves to \(0.10 \mathrm{~m}\). At this new distance, the speed of the block is \(2.80 \mathrm{~m} / \mathrm{s}\). (a) What is the tension in the cord in the original situation, when the block has speed \(v=0.70 \mathrm{~m} / \mathrm{s} ?\) (b) What is the tension in the cord in the final situation. when the block has speed \(v=2.80 \mathrm{~m} / \mathrm{s} ?\) (c) How much work was done by the person who pulled on the cord?

BIO Power of the Human Heart. The human heart is a powerful and extremely reliable pump. Each day it takes in and discharges about \(7500 \mathrm{~L}\) of blood. Assume that the work done by the heart is equal to the work required to lift this amount of blood a height equal to that of the average American woman ( \(1.63 \mathrm{~m}\) ). The density (mass per unit volume) of blood is \(1.05 \times 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\). (a) How much work does the heart do in a day? (b) What is the heart's power output in watts?

To stretch an ideal spring \(3.00 \mathrm{~cm}\) from its unstretched length, \(12.0 \mathrm{~J}\) of work must be done. (a) What is the force constant of this spring? (b) What magnitude force is needed to stretch the spring 3.00 \(\mathrm{cm}\) from its unstretched length? (c) How much work must be done to compress this spring \(4.00 \mathrm{~cm}\) from its unstretched length, and what force is needed to compress it this distance?

You are a member of an Alpine Rescue Team. You must project a box of supplies up an incline of constant slope angle \(\alpha\) so that it reaches a stranded skier who is a vertical distance \(h\) above the bottom of the incline. The incline is slippery, but there is some friction present, with kinetic friction coefficient \(\mu_{\mathrm{k}}\). Use the work-energy theorem to calculate the minimum speed you must give the box at the bottom of the incline so that it will reach the skier. Express your answer in terms of \(g, h, \mu_{k},\) and \(\alpha\)

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