/*! 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 68 A firefighting crew uses a water... [FREE SOLUTION] | 91Ó°ÊÓ

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A firefighting crew uses a water cannon that shoots water at 25.0 m/s at a fixed angle of 53.0\(^\circ\) above the horizontal. The firefighters want to direct the water at a blaze that is 10.0 m above ground level. How far from the building should they position their cannon? There are \(two\) possibilities; can you get them both? (\(Hint\): Start with a sketch showing the trajectory of the water.)

Short Answer

Expert verified
The cannon can be positioned at either 8.85 meters or 51.6 meters from the building.

Step by step solution

01

Initial Setup

Before starting the calculations, sketch a trajectory diagram of the water to help visualize the path. The trajectory is a parabola because the angle is above the horizontal due to projectile motion. This will aid in distinguishing the two points of height that the water can reach before descending, meeting the target value of 10.0 m.
02

Determine Horizontal and Vertical Components of Velocity

Decompose the initial velocity of 25.0 m/s into horizontal and vertical components. The horizontal component is \(v_{x} = 25.0 \cos 53.0^{\circ}\) and the vertical component is \(v_{y} = 25.0 \sin 53.0^{\circ}\). Calculating these, we get \(v_{x} \approx 15.0 \text{ m/s}\) and \(v_{y} \approx 20.0 \text{ m/s}\).
03

Write the Equation of Motion for Vertical Displacement

The vertical motion equation considering the initial velocity, gravity, and time is: \(y = v_{y}t - \frac{1}{2}gt^2\). Set \(y = 10.0\) m and solve for time \(t\), using \(g = 9.8\text{ m/s}^2\). This gives us a quadratic equation: \(10 = 20t - 4.9t^2\).
04

Solve the Quadratic Equation for Time

Solve the quadratic equation \(4.9t^2 - 20t + 10 = 0\) using the quadratic formula: \(t = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), where \(a = 4.9\), \(b = -20\), and \(c = 10\). This yields two solutions for time: \(t_1 \approx 0.59\text{ s} \) and \(t_2 \approx 3.44\text{ s}\).
05

Calculate Horizontal Distances

Using the calculated times, determine the horizontal distances using the formula: \(x = v_{x}t\). For \(t_1 = 0.59\text{ s}\), \(x_1 = 15.0 \times 0.59 \approx 8.85\text{ m}\). For \(t_2 = 3.44\text{ s}\), \(x_2 = 15.0 \times 3.44 \approx 51.6\text{ m}\).
06

Conclusion

Based on the solutions for the times, the firefighting crew can position their cannon either 8.85 meters or 51.6 meters away from the building to hit the target height of 10.0 meters with the water stream.

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Key Concepts

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

horizontal and vertical components
In projectile motion, understanding the horizontal and vertical components is key to solving any related problems. Imagine you have a water cannon like in the exercise. It shoots water at a certain speed and angle. This speed, known as initial velocity, can be broken down into two parts, horizontal and vertical, using trigonometry.
The horizontal component (\( v_x \)) is responsible for the forward movement of the projectile. It can be found using the cosine of the angle with the formula: \( v_x = v_{initial} \cos{\theta} \). The vertical component (\( v_y \)), however, affects how high the projectile will go and is calculated with the sine of the angle: \( v_y = v_{initial} \sin{\theta} \).
  • For example, with a velocity of 25 m/s at a 53-degree angle, the horizontal component is about 15 m/s.
  • The vertical component is around 20 m/s.
These decomposed values help us understand and predict the motion path, breaking it into manageable sections.
trajectory of a projectile
Once we know our horizontal and vertical components, we can predict the path or trajectory of the projectile — in this case, the water stream. In physics, this path forms a parabolic shape due to gravity's pull.
The initial speed sends the projectile upward, but gravity slows it down until it stops for a brief moment at its highest point. Then, it pulls the projectile back down.
Visualizing the trajectory helps in planning where the water stream needs to land. The exercise above attempts to find out where to position the cannon, ensuring the water reaches a precise height. By sketching a diagram, the arc of the water can be seen clearly.
  • This helps firefighters determine two points at height 10m where the stream will pass through: one on the way up, and another on the way down.
This parabolic path highlights how both angles of launch and speed influence the outcome of projectile motion.
quadratic equation in physics
Quadratic equations are mathematical representations often used to solve physics problems involving projectile motion. In the exercise, the vertical position is described by a quadratic equation, highlighting how changes in time affect the projectile's height.
The formula used is \( y = v_y t - \frac{1}{2}gt^2 \). We know our target height is 10 m. By substituting known values, we find \( 10 = 20t - 4.9t^2 \). This forms a quadratic equation, \( 4.9t^2 - 20t + 10 = 0 \), that can be solved using the quadratic formula.
Solving it allows us to find two different times when the projectile reaches this height:
  • \( t_1 \approx 0.59 \ ext{ s} \)
  • \( t_2 \approx 3.44 \ ext{ s} \)
These solutions correspond to two possible distances from the building where the cannon can be positioned. The quadratic nature of the equation reflects the reality of motion influenced by gravity, displaying both ascend and descend points within the trajectory.

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Most popular questions from this chapter

A faulty model rocket moves in the \(xy\)-plane (the positive \(y\)-direction is vertically upward). The rocket's acceleration has components \(a_x(t) = \alpha t^2\) and \(a_y(t) = \beta - \gamma t\), where \(\alpha = 2.50 m/s^4, \beta = 9.00 m/s^2,\) and \(\gamma = 1.40 m/s^3\). At \(t = 0\) the rocket is at the origin and has velocity \(\vec{v}_0=v_0\hat{i} + v_{0y}\hat{j}\) with \(v_{0x}\) = 1.00 m/s and \(v_{0y}\) = 7.00 m/s. (a) Calculate the velocity and position vectors as functions of time. (b) What is the maximum height reached by the rocket? (c) What is the horizontal displacement of the rocket when it returns to \(y = 0\)?

A projectile thrown from a point \(P\) moves in such a way that its distance from \(P\) is always increasing. Find the maximum angle above the horizontal with which the projectile could have been thrown. Ignore air resistance.

A rookie quarterback throws a football with an initial upward velocity component of 12.0 m/s and a horizontal velocity component of 20.0 m/s. Ignore air resistance. (a) How much time is required for the football to reach the highest point of the trajectory? (b) How high is this point? (c) How much time (after it is thrown) is required for the football to return to its original level? How does this compare with the time calculated in part (a)? (d) How far has the football traveled horizontally during this time? (e) Draw \(x-t, y-t, v_x-t\), and \(v_y-t\) graphs for the motion.

The nose of an ultralight plane is pointed due south, and its airspeed indicator shows 35 m/s. The plane is in a 10-m/s wind blowing toward the southwest relative to the earth. (a) In a vectoraddition diagram, show the relationship of \(\vec{v}_{P/E}\) (the velocity of the plane relative to the earth) to the two given vectors. (b) Let \(x\) be east and y be north, and find the components of \(\vec{v} _{P/E}\). (c) Find the magnitude and direction of \(\vec{v} _{P/E}\).

Firemen use a high-pressure hose to shoot a stream of water at a burning building. The water has a speed of 25.0 m/s as it leaves the end of the hose and then exhibits projectile motion. The firemen adjust the angle of elevation \(\alpha\) of the hose until the water takes 3.00 s to reach a building 45.0 m away. Ignore air resistance; assume that the end of the hose is at ground level. (a) Find \(\alpha\). (b) Find the speed and acceleration of the water at the highest point in its trajectory. (c) How high above the ground does the water strike the building, and how fast is it moving just before it hits the building?

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