/*! 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 37 The human body can safely tolera... [FREE SOLUTION] | 91Ó°ÊÓ

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The human body can safely tolerate a vertical acceleration \(9.00\) times that due to gravity. With what minimum radius of curvature may a pilot safely turn the plane upward at the end of a dive if the plane's speed is \(770 \mathrm{~km} / \mathrm{h}\) ?

Short Answer

Expert verified
The minimum radius of curvature is approximately 518 meters.

Step by step solution

01

Understanding the Problem

We need to find the minimum radius of curvature for the pilot's safe turn during an upward motion at the end of a dive. The plane's speed is given as 770 km/h, and the maximum tolerated acceleration is 9 times the gravitational acceleration, i.e., 9g.
02

Converting Units

Convert the speed from km/h to m/s for easier calculation: \[ 770 \text{ km/h} = \frac{770 \times 1000}{3600} \text{ m/s} \approx 213.89 \text{ m/s} \]
03

Applying the Centripetal Acceleration Formula

The centripetal acceleration formula is \( a = \frac{v^2}{r} \). We have the acceleration as \( 9g = 9 \times 9.81 \text{ m/s}^2 = 88.29 \text{ m/s}^2 \). Here, \( v = 213.89 \text{ m/s} \) and we need to solve for \( r \).
04

Solving for the Radius

Rearrange the centripetal acceleration formula to solve for \( r \):\[ r = \frac{v^2}{a} = \frac{(213.89)^2}{88.29} \]
05

Calculating the Radius

Substitute the known values into the equation:\[ r = \frac{45776.11}{88.29} \approx 518.39 \text{ meters} \]
06

Rounding for Precision

Round the result to a reasonable significant figure: The minimum radius of curvature is approximately 518 meters.

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Key Concepts

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

Centripetal Acceleration
When an object moves along a curved path, it experiences centripetal acceleration, which is directed toward the center of the curvature. It helps keep the object in its circular path. Imagine swinging a ball on a string in a circle: the string pulls the ball inward, preventing it from flying off. Similarly, when a plane turns upward at the end of a dive, the centripetal force is necessary to alter its direction.
For any object moving at a speed, say a plane flying at 213.89 m/s, the required centripetal acceleration can be calculated using the formula:
  • \( a = \frac{v^2}{r} \)
Here, \( v \) is the object's speed and \( r \) is the radius of curvature. If the pilot pulls too suddenly, exceeding safe acceleration limits, there might be adverse effects on both the pilot and the aircraft. Hence, understanding and calculating centripetal acceleration is crucial for safe maneuvers.
Gravitational Acceleration
Gravitational acceleration is the acceleration due to the force of gravity acting on an object. On Earth, this value is approximately \( 9.81 \, \text{m/s}^2 \). The human body, especially in aviation scenarios, can typically withstand more than just this base gravitational figure.
When a pilot performs high-speed maneuvers like pulling out of a dive, they can be subjected to accelerations many times greater than gravity, often referred to as 'g-forces'. In this scenario, the pilot can safely handle up to 9 times gravitational acceleration, equal to \( 9 \times 9.81 = 88.29 \, \text{m/s}^2 \). Calculating this maximum safe limit is vital to avoid dangerous stress on the pilot's body. Understanding these limits ensures that both pilots and passengers travel safely without experiencing undue stress.
Unit Conversion
Unit conversion is a critical step in solving physics problems, as it ensures consistency across calculations. In this exercise, speed given in kilometers per hour (km/h) needs to be converted to meters per second (m/s), as it aligns with the units for acceleration \( \text{m/s}^2 \).
The conversion involves adjusting the unit scale from hours to seconds, and from kilometers to meters.
  • Convert speed using: \(770 \, \text{km/h} = \frac{770 \times 1000}{3600} \, \text{m/s} \approx 213.89 \, \text{m/s} \)
This conversion is essential for ensuring your calculations align and that results are both understandable and coherent. Errors in unit conversion can lead to inaccurate results, so it's paramount to perform these steps correctly.
Radius of Curvature
The radius of curvature is a measure of the sharpness of a curve or arc. In aviation, it dictates how smoothly a plane can turn or change direction without exceeding safe acceleration limits. A larger radius results in a gentler turn, while a smaller radius demands quicker directional change.
For a plane turning at the end of a dive, calculating the minimum radius of curvature ensures the plane does not exceed tolerable g-forces. This radius can be found from the centripetal acceleration formula rearranged as:
  • \( r = \frac{v^2}{a} \)
Given a speed \( v \) of 213.89 m/s and acceleration \( a \) of \( 88.29 \, \text{m/s}^2 \), substitute to find \( r \):
  • \( r = \frac{(213.89)^2}{88.29} \approx 518 \) meters
This computation helps in designing and executing flight paths that stay within safety limits, reducing risks.

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Most popular questions from this chapter

What is the maximum speed at which a car can round a curve of \(25-\mathrm{m}\) radius on a level road if the coefficient of static friction between the tires and road is \(0.80\) ? The radial force required to keep the car in the curved path (the centripetal force) is supplied by friction between the tires and the road. If the mass of the car is \(m\), the maximum friction force (which is the centripetal force) equals \(\mu, F_{N}\) or \(0.80 \mathrm{mg}\), this arises when the car is on the verge of skidding sideways. Therefore, the maximum speed is given by $$ \frac{m v^{2}}{r}=0.80 \mathrm{mg} \quad \text { or } \quad v=\sqrt{0.80 \mathrm{gr}}=\sqrt{(0.80)\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(25 \mathrm{~m})}=14 \mathrm{~m} / \mathrm{s} $$

A \(200-\mathrm{g}\) object is tied to the end of a cord and whirled in a horizontal circle of radius \(1.20 \mathrm{~m}\) at a constant \(3.0 \mathrm{rev} / \mathrm{s}\). Assume that the cord is horizontal - that is, that gravity can be neglected. Determine ( \(a\) ) the centripetal acceleration of the object and ( \(b\) ) the tension in the cord. (a) The object is not accelerating tangentially to the circle but is undergoing a radial, or centripetal, acceleration given by $$ a_{c}=\frac{v^{2}}{r}=r \omega^{2} $$ where \(\omega\) must be in \(\mathrm{rad} / \mathrm{s}\). Since \(3.0 \mathrm{rev} / \mathrm{s}=6.0 \pi \mathrm{rad} / \mathrm{s}\), $$ a_{C}=(1.20 \mathrm{~m})(6.0 \pi \mathrm{rad} / \mathrm{s})^{2}=426 \mathrm{~m} / \mathrm{s}^{2}=0.43 \mathrm{~km} / \mathrm{s}^{2} $$ (b) To cause the acceleration found in \((a)\), the cord must pull on the \(0.200-\mathrm{kg}\) mass with a centripetal force given by $$ F_{C}=m a_{C}=(0.200 \mathrm{~kg})\left(426 \mathrm{~m} / \mathrm{s}^{2}\right)=85 \mathrm{~N} $$ This is the tension in the cord

A mass of \(1.5 \mathrm{~kg}\) out in space moves in a circle of radius \(25 \mathrm{~cm}\) at a constant \(2.0 \mathrm{rev} / \mathrm{s}\). Calculate \((a)\) the tangential speed, (b) the acceleration, and ( \(c\) ) the required centripetal force for the motion.

A car wheel \(30 \mathrm{~cm}\) in radius is tuming at a rate of \(8.0 \mathrm{rev} / \mathrm{s}\) when the car begins to slow uniformly to rest in \(\mathrm{A}\) time of \(14 \mathrm{~s}\). Find the number of revolutions made by the wheel and the distance the car goes in the \(14 \mathrm{~s}\).

A thin string wound on the rim of a wheel \(20 \mathrm{~cm}\) in diameter is pulled out at a rate of \(75 \mathrm{~cm} / \mathrm{s}\) causing the wheel to rotate about its central axis. Through how many revolutions will the wheel have turned by the time that \(9.0 \mathrm{~m}\) of string have been unwound? How long will it take?

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