Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A 1000.-kg cannon shoots a 30.0-kg shell at an angle of \(25.0^{\circ}\) above the horizontal and a speed of \(500 . \mathrm{m} / \mathrm{s}\) with respect to the ground. What is the recoil velocity of the cannon?

Short Answer

Expert verified
A) -13.62 m/s B) 13.62 m/s C) -453.97 m/s D) 453.97 m/s

Step by step solution

01

Identify the initial momentum of the system

Before the cannon is fired, it is stationary along with the shell. Therefore, their initial momentum is zero.
02

Determine the momentum of the fired shell

To find the momentum of the shell after being fired from the cannon, we can use the equation: $$ \text{momentum} = \text{mass} \times \text{velocity} $$ Since the shell is fired at a \(25.0^{\circ}\) angle above the horizontal, we only need to consider the horizontal component of its velocity. Using trigonometry, we get: $$ v_{\text{horizontal}} = |\vec{v}| \times \cos(\theta) $$ Now, we can plug in the values: $$ v_{\text{horizontal}} = 500 \ \text{m/s} \times \cos(25^\circ) $$ $$ v_{\text{horizontal}} \approx 453.97 \ \text{m/s} $$ Then, calculate the momentum: $$ \text{momentum}_{\text{shell}} = 30.0 \ \text{kg} \times 453.97 \ \text{m/s} $$ $$ \text{momentum}_{\text{shell}} \approx 13619.1 \ \text{kg} \cdot \text{m/s} $$
03

Apply the conservation of momentum principle

Now that we have the momentum of the fired shell, we can apply the conservation of momentum principle: $$ \text{momentum}_{\text{initial}} = \text{momentum}_{\text{final}} $$ In this case, the initial momentum is zero. Thus: $$ 0 = \text{momentum}_{\text{shell}} + \text{momentum}_{\text{cannon}} $$ Now we will solve for the momentum of the cannon: $$ \text{momentum}_{\text{cannon}} = -\text{momentum}_{\text{shell}} $$ $$ \text{momentum}_{\text{cannon}} \approx -13619.1 \ \text{kg} \cdot \text{m/s} $$
04

Calculate the recoil velocity of the cannon

Finally, we need to find the recoil velocity of the cannon using its momentum: $$ \text{velocity} = \frac{\text{momentum}}{\text{mass}} $$ Now, plug in the values: $$ v_{\text{recoil}} = \frac{-13619.1 \ \text{kg} \cdot \text{m/s}}{1000 \ \text{kg}} $$ $$ v_{\text{recoil}} \approx -13.62 \ \text{m/s} $$ The recoil velocity of the cannon is approximately -13.62 m/s (the negative sign indicates that the direction of the velocity is opposite to the direction of the fired shell).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Conservation of Momentum
When we think about the recoil velocity of the cannon, we are looking at a clear example of the conservation of momentum in action. The law of conservation of momentum states that in a closed system with no external forces, the total momentum before an event must equal the total momentum after the event.

In the case of our cannon and cannonball, before the cannon is fired, both the cannon and shell have zero momentum because they are not moving. As the cannonball is fired and gains momentum in one direction, the cannon itself must gain an equal amount of momentum in the opposite direction. This explains the recoil or backward movement that we observe in the cannon.

Grasping this concept is crucial because it not only applies to cannons but to any system where objects interact and exert forces on each other, such as cars in a collision or athletes pushing off one another in sports.
Projectile Motion
Projectile motion comes into play when an object is thrown or projected into the air, moving under the influence of gravity while continuing its original motion at the same time. This type of motion is two-dimensional and has both vertical and horizontal components that can be calculated separately.

In our example, the shell is projected at an angle, which means it has an initial horizontal velocity and a vertical velocity. The horizontal velocity affects how far the shell with travel, while the vertical velocity will determine the height of its arc. By understanding projectile motion, students can predict the trajectories of objects and solve for various factors, such as range, maximum height, and time of flight, using principles of kinematics.
Trigonometry in Physics
Trigonometry is a branch of mathematics that's essential for breaking down and understanding forces and movements in physics, especially in two-dimensional motion like projectile motion.

In the case of the cannon firing the shell, we use trigonometry to resolve the shell's velocity into horizontal and vertical components. Knowing the angle of \(25.0^\circ\) and the initial speed, we calculate the horizontal component of the velocity using the cosine function. Such calculations are common in physics problems, allowing us to understand and predict how different forces and velocities impact the movement of objects in different directions.
Momentum
Momentum is a vector quantity that is central to the laws of motion. It is the product of an object's mass and velocity, and it describes the quantity of motion an object has.

In this exercise, when the cannon fires a shell, the momentum of the shell can be calculated using its mass and the horizontal component of its velocity, as derived from trigonometry. The larger an object's momentum, the harder it is to stop. Momentum has both magnitude and direction, which means that the momentum of the cannon after firing is equal in magnitude to the shell's momentum but in the opposite direction. This concept helps explain various phenomena, from vehicle dynamics in engineering to sports where collisions and changes in motion occur.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Suppose you place an old fashioned hourglass, with sand in the bottom, on a very sensitive analytical balance to determine its mass. You then turn it over (handling it with very clean gloves) and place it back on the balance. You want to predict whether the reading on the balance will be less than, greater than, or the same as before. What do you need to calculate to answer this question? Explain carefully what should be calculated and what the results would imply. You do not need to attempt the calculation.

The center of mass of the Sun and Jupiter is located a) exactly at the center of the Sun. b) near the center of the Sun. c) exactly at the center of Jupiter. d) near the center of Jupiter. e) halfway between the Sun and Jupiter.

Two point masses are located in the same plane. The distance from mass 1 to the center of mass is \(3.0 \mathrm{~m} .\) The distance from mass 2 to the center of mass is \(1.0 \mathrm{~m}\). What is \(m_{1} / m_{2}\), the ratio of mass 1 to mass 2 ? a) \(3 / 4\) b) \(4 / 3\) c) \(4 / 7\) d) \(7 / 4\) c) \(4 / 7\) d) \(7 / 4\)

Many nuclear collisions studied in laboratories are analyzed in a frame of reference relative to the laboratory. A proton, with a mass of \(1.6726 \cdot 10^{-27} \mathrm{~kg}\) and traveling at a speed of \(70.0 \%\) of the speed of light, \(c\) collides with a tin- \(116\left({ }^{116} \mathrm{Sn}\right)\) nucleus with a mass of \(1.9240 \cdot 10^{-25} \mathrm{~kg} .\) What is the speed of the center of mass with respect to the laboratory frame? Answer in terms of \(c\), the speed of light.

A man standing on frictionless ice throws a boomerang, which returns to him. Choose the correct statement: a) Since the momentum of the man-boomerang system is conserved, the man will come to rest holding the boomerang at the same location from which he threw it. b) It is impossible for the man to throw a boomerang in this situation. c) It is possible for the man to throw a boomerang, but because he is standing on frictionless ice when he throws it, the boomerang cannot return. d) The total momentum of the man-boomerang system is not conserved, so the man will be sliding backward holding the boomerang after he catches it.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free