/*! 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 98 An alert hiker sees a boulder fa... [FREE SOLUTION] | 91Ó°ÊÓ

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An alert hiker sees a boulder fall from the top of a distant cliff and notes that it takes 1.30 s for the boulder to fall the last third of the way to the ground. You may ignore air resistance. (a) What is the height of the cliff in meters? (b) If in part (a) you get two solutions of a quadratic equation and you use one for your answer, what does the other solution represent?

Short Answer

Expert verified
The cliff is approximately 60.5 meters high. The other solution is nonphysical and can be discarded.

Step by step solution

01

Identify Known Values

We know the time it took for the boulder to fall the last third of the distance, which is 1.30 seconds. We also know that free-fall acceleration is given by gravity, so we use the constant acceleration due to gravity, \( g = 9.81 \, \text{m/s}^2 \). This problem involves calculating the total height of the cliff.
02

Set Up Equations of Motion

Let \( h \) be the total height of the cliff, so the boulder falls \( \frac{h}{3} \) in the last 1.30 seconds. For the entire fall, the boulder's motion can be described using the equation for distance under constant acceleration: \[ s = v_0t + \frac{1}{2}gt^2 \] where \( s \) is the distance fallen, \( v_0 \) is the initial velocity for each section of the fall, and \( t \) is the time.
03

Find Time of Total Fall

Let \( t_1 \) be the total time taken to fall the whole cliff height \( h \). We need to express \( t_1 \) in terms of \( h \), utilizing the equation: \[ h = \frac{1}{2}g t_1^2 \] thus \( t_1 = \sqrt{\frac{2h}{g}} \).
04

Describe Last Third Falls

For the last third of the distance, express initial velocity \( v_0 \) at the start of this last section using \( t_1 - 1.3 \) (the time needed to fall the first \( \frac{2}{3}h \)). From the first \( \frac{2}{3} \) fall: \[ \frac{2h}{3} = \frac{1}{2}g (t_1 - 1.3)^2 \].
05

Solve for Total Height

We now have two equations: one for the full height and one for the initial velocity of the final section. Use \( h = \frac{1}{2}g t_1^2 \) and substitute \( v_0 \) from part of the motion: \[ \frac{h}{3} = v_0 \cdot 1.3 + \frac{1}{2}g(1.3)^2 \]. These equations involve solving a quadratic in \( h \).
06

Quadratic Formula Calculation

Combine the equations and use the quadratic formula to find \( h \): \[ h = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \] where these variables relate to the combined equation involving \( h \). You should analyze which solution matches the conditions of the problem.
07

Analyze Solutions

Solving the quadratic, you find two possible values for \( h \). One is typically realistic (positive height) for the cliff, and the other might represent a nonphysical solution in this context (possibly a negative time or height due to nature of equation).

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Key Concepts

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

Gravity
Gravity is a fundamental force that gives us weight and makes objects fall toward the Earth. It's the reason we stay grounded and why things don't just float away into space. On Earth, this force causes an acceleration known as "acceleration due to gravity," represented by the symbol \( g \).

For our calculations in most physics problems, gravity is considered to be \( 9.81 \, \text{m/s}^2 \). This means any object under free fall in a vacuum would accelerate at roughly 9.81 meters per second squared.

In physics problems involving gravity, such as the boulder falling from a cliff, we assume gravitational acceleration is constant. This simplifies the problem, allowing us to apply equations of motion to calculate various aspects of the object's fall.
Equations of Motion
Equations of motion describe the behavior of objects in motion. They're crucial when analyzing problems involving accelerating objects. In this scenario, the equations help us understand the boulder's descent from the cliff.

The primary equation involved here is: \[ s = v_0t + \frac{1}{2}gt^2 \]

- \( s \) is the distance fallen,
- \( v_0 \) is the initial velocity,
- \( t \) is the time, and
- \( g \) is the gravitational acceleration.

This simple formula allows you to calculate either the distance an object travels or the time it takes, when it's in free fall. Plus, by rearranging the formula, you can find out how fast the object was going initially. These pieces are important for determining both the total height of the cliff and the details of the boulder's final descent.
Quadratic Equations
In this problem, the use of quadratic equations comes into play when solving for the height of the cliff. When you combine different parts of the motion in their equations, you often end up with a quadratic equation in physics problems.

A typical quadratic equation looks like: \( ax^2 + bx + c = 0 \). Solving such equations involves finding the values of \( x \) that satisfy the equation. This is done using the quadratic formula: \[ x = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \]

- \( a \), \( b \), and \( c \) are coefficients that come from the expanded equations.

In the case of the boulder, finding the height involves plugging these into the formula to get two potential answers. One solution often matches the physical scenario (a positive height), while the other might not (could be negative height or time, which doesn't make sense physically). Always pick the solution that fits the real-world context.
Free Fall
Free fall is an important concept in physics. It's when an object is only acted upon by gravity, with no other forces like air resistance altering its path. In our exercise, the falling boulder is a perfect example of free fall.

This simplifies calculations since the only acceleration is due to gravity. An object in free fall accelerates downward at a constant rate of \( 9.81 \, \text{m/s}^2 \). Understanding this allows us to apply the equations of motion formidably.

- In the real world, few objects are in true free fall due to the presence of air.
- In physics problems, ignoring air resistance lets us focus solely on gravitational effects.

Grasping the concept of free fall helps break down more complicated motion scenarios in physics, serving as the foundation for many more advanced topics.

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Most popular questions from this chapter

During launches, rockets often discard unneeded parts. A certain rocket starts from rest on the launch pad and accelerates upward at a steady 3.30 \(\mathrm{m} / \mathrm{s}^{2}\) . When it is 235 \(\mathrm{m}\) above the launch pad, it discards a used fuel canister by simply disconnecting it. Once it is disconnected, the only force acting on the canister is gravity (air resistance can be ignored). (a) How high is the rocket when the canister hits the launch pad, assuming that the rocket does not change its acceleration? (b) What total distance did the canister travel between its release and its crash onto the launch pad?

CALC A car is stopped at a traffic light. It then travels along a straight road so that its distance from the light is given by \(x(t)=b t^{2}-c t^{3},\) where \(b=2.40 \mathrm{m} / \mathrm{s}^{2}\) and \(c=0.120 \mathrm{m} / \mathrm{s}^{3} .\) (a) Calculate the average velocity of the car for the time interval \(t=0\) to \(t=10.0\) s. (b) Calculate the instantaneous velocity of the car at \(t=0, t=5.0 \mathrm{s},\) and \(t=10.0 \mathrm{s}\) . (c) How long after starting from rest is the car again at rest?

A car travels in the \(+x\) -direction on a straight and level road. For the first 4.00 s of its motion, the average velocity of the car is \(v_{\mathrm{av}-x}=6.25 \mathrm{m} / \mathrm{s} .\) How far does the car travel in 4.00 \(\mathrm{s}\) ?

The acceleration of a particle is given by \(a_{x}(t)=\) \(-2.00 \mathrm{m} / \mathrm{s}^{2}+\left(3.00 \mathrm{m} / \mathrm{s}^{3}\right) t .\) (a) Find the initial velocity \(v_{0 x}\) such that the particle will have the same \(x\) -coordinate at \(t=4.00 \mathrm{s}\) as it had at \(t=0 .\) (b) What will be the velocity at \(t=4.00\) s?

Are We Martians? It has been suggested, and not facetiously, that life might have originated on Mars and been carried to the earth when a meteor hit Mars and blasted pieces of rock (perhaps containing primitive life) free of the surface. Astronomers know that many Martian rocks have come to the earth this way. (For information on one of these, search the Internet for "ALH \(84001 . "\) ') One objection to this idea is that microbes would have to undergo an enormous lethal acceleration during the impact. Let us investigate how large such an acceleration might be. To escape Mars, rock fragments would have to reach its escape velocity of \(5.0 \mathrm{km} / \mathrm{s},\) and this would most likely happen over a distance of about 4.0 \(\mathrm{m}\) during the meteor impact. (a) What would be the acceleration ( in \(\mathrm{m} / \mathrm{s}^{2}\) and \(g^{\prime} \mathrm{s}\)) of such a rock fragment, if the acceleration is constant? (b) How long would this acceleration last? (c) In tests, scientists have found that over 40\(\%\) of Bacillius subtilis bacteria survived after an acceleration of \(450,000 g .\) In light of your answer to part (a), can we rule out the hypothesis that life might have been blasted from Mars to the earth?

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