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(I) A jet plane traveling \(1890 \mathrm{~km} / \mathrm{h}(525 \mathrm{~m} / \mathrm{s})\) pulls out of a dive by moving in an arc of radius \(4.80 \mathrm{~km} .\) What is the plane's acceleration in \(g\) 's?

Short Answer

Expert verified
The plane's acceleration is approximately 5.86 g's.

Step by step solution

01

Understand the Circumstances

The plane is traveling at a velocity of \( v = 525 \text{ m/s} \). It moves in a circular path of radius \( r = 4800 \text{ m} \) (converted from kilometers to meters). We need to find the centripetal acceleration \( a \).
02

Use the Centripetal Acceleration Formula

The formula for centripetal acceleration is given by \( a = \frac{v^2}{r} \). Substitute the given velocity and radius into this formula: \[ a = \frac{(525 \text{ m/s})^2}{4800 \text{ m}} \].
03

Calculate the Centripetal Acceleration

Perform the calculations for \( a \): \( a = \frac{275625}{4800} = 57.43 \text{ m/s}^2 \). The plane's acceleration is found to be \( 57.43 \text{ m/s}^2 \).
04

Convert the Acceleration to g's

The unit \( g \) corresponds to the acceleration due to gravity, which is approximately \( 9.81 \text{ m/s}^2 \). We convert the calculated acceleration to g's by dividing by \( 9.81 \text{ m/s}^2 \):\[ \text{acceleration in } g\text{'s} = \frac{57.43 \text{ m/s}^2}{9.81 \text{ m/s}^2} \approx 5.86 \text{ g} \].

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Key Concepts

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

Jet Plane Motion
In the context of this exercise, understanding the motion of a jet plane is crucial. Jet planes are remarkable machines capable of reaching incredible speeds surpassing most conventional aircraft. However, with these high velocities come unique challenges, particularly related to the way they maneuver.

When a jet travels, especially during complex maneuvers like pulling out of a dive, it often moves in what we refer to as circular motion. In such instances, centripetal forces come into play to ensure the plane remains on its intended curved path. An easy way to visualize this is by picturing a plane traveling at a constant speed but consistently changing direction. This directional change is what creates a circular motion.

For a jet plane, the radius of the turn, or arc, is a vital aspect. In our example, the jet plane is moving with a radius of 4.80 kilometers during its dive maneuver. This radius, combined with the velocity, determines the centripetal acceleration, which needs to be calculated accurately for safety and performance reasons. Factors like these reinforce the complexities involved in aviation physics.
Circular Motion
Circular motion is fundamental to understanding scenarios like a jet plane pulling out of a dive. It describes an object's movement along a circular path, which involves constantly changing direction, despite maintaining a uniform speed. This kind of motion is governed by centripetal acceleration, crucial for keeping an object moving in a circle.

The formula for centripetal acceleration is expressed as:
  • \[ a = \frac{v^2}{r} \]
where \( v \) represents the velocity and \( r \) represents the radius of the circular path. It's important to comprehend that despite a constant speed, the velocity vector is always changing direction as the object moves along the curved path. This change in direction is precisely what provides the centripetal acceleration required.

In the case of our jet plane, given a velocity of 525 m/s and a radius of 4800 meters, utilizing the formula \( a = \frac{v^2}{r} \), helps us determine a centripetal acceleration of 57.43 m/s². This underlines the significant role of centripetal forces in circular motion, ensuring stability and precision in paths taken by fast-moving objects like jet planes.
Acceleration Conversion
Sometimes, quantities must be expressed in different units to provide better insight or understanding. In physics, understanding acceleration in terms of g-force is quite common, especially in aviation and astronautics. G-force, denoted by the unit \( g \), is the measure of acceleration experienced as weight.

To convert an acceleration from meters per second squared (m/s²) into g's, you divide it by the standard acceleration due to gravity, approximately \( 9.81 \, \text{m/s}^2 \). This conversion simplifies the concept into something more intuitive by comparing it to the familiar force of gravity experienced every day.

In our exercise, after determining the plane's centripetal acceleration (57.43 m/s²), we convert it into g's:
  • \[ \text{Acceleration in } g\text{'s} = \frac{57.43 \, \text{m/s}^2}{9.81 \, \text{m/s}^2} \approx 5.86 \, g \]
This conversion provides pilots and engineers a straightforward measurement of how intense the acceleration is compared to what we experience due to gravity, which is essential for assessing both pilot safety and structural integrity of the aircraft.

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Most popular questions from this chapter

(II) A box is given a push so that it slides across the floor. How far will it go, given that the coefficient of kinetic friction is 0.15 and the push imparts an initial speed of \(3.5 \mathrm{~m} / \mathrm{s} ?\)

A \(2.0-\mathrm{kg}\) silverware drawer does not slide readily. The owner gradually pulls with more and more force, and when the applied force reaches \(9.0 \mathrm{~N}\), the drawer suddenly opens, throwing all the utensils to the floor. What is the coefficient of static friction between the drawer and the cabinet?

A \(72-\mathrm{kg}\) water skier is being accelerated by a ski boat on a flat ("glassy") lake. The coefficient of kinetic friction between the skier's skis and the water surface is \(\mu_{\mathrm{k}}=0.25\) (Fig. \(5-55)\). (a) What is the skier's acceleration if the rope pulling the skier behind the boat applies a horizontal tension force of magnitude \(F_{\mathrm{T}}=240 \mathrm{~N}\) to the skier \(\left(\theta=0^{\circ}\right) ?\) (b) What is the skier's horizontal acceleration if the rope pulling the skier exerts a force of \(F_{\mathrm{T}}=240 \mathrm{~N}\) on the skier at an upward angle \(\theta=12^{\circ} ?\) (c) Explain why the skier's acceleration in part ( \(b\) ) is greater than that in part ( \(a\) ).

(II) \((a)\) Show that the minimum stopping distance for an automobile traveling at speed \(v\) is equal to \(v^{2} / 2 \mu_{\mathrm{s}} g,\) where \(\mu_{\mathrm{s}}\) is the coefficient of static friction between the tires and the road, and \(g\) is the acceleration of gravity. (b) What is this distance for a \(1200-\mathrm{kg}\) car traveling \(95 \mathrm{~km} / \mathrm{h}\) if \(\mu_{\mathrm{s}}=0.65 ?\) (c) What would it be if the car were on the Moon (the acceleration of gravity on the Moon is about \(g / 6\) ) but all else stayed the same?

(I) What is the maximum speed with which a \(1200-\mathrm{kg}\) car can round a turn of radius \(80.0 \mathrm{~m}\) on a flat road if the coefficient of friction between tires and road is \(0.65 ?\) Is this result independent of the mass of the car?

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