/*! 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 48 A rifle shoots a 4.20 g bullet o... [FREE SOLUTION] | 91Ó°ÊÓ

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A rifle shoots a 4.20 g bullet out of its barrel. The bullet has a muzzle velocity of 965 \(\mathrm{m} / \mathrm{s}\) just as it leaves the barrel. Assuming a constant horizontal acceleration over a distance of 45.0 \(\mathrm{cm}\) starting from rest, with no friction between the bullet and the barrel, (a) what force does the rifle exert on the bullet while it is in the barrel? (b) Draw a free-body diagram of the bullet (i) while it is in the barrel and (ii) just after it has left the barrel. (c) How many \(g^{\prime}\) s of acceleration does the rifle give this bullet? (d) For how long a time is the bullet in the barrel?

Short Answer

Expert verified
The force on the bullet is 4355 Newtons. The bullet's acceleration is 214,285 g's. Time in the barrel is 0.001 s.

Step by step solution

01

Convert Units

First, convert the given quantities to SI units. The mass of the bullet is given as 4.20 g, which is equal to 0.00420 kg because there are 1000 grams in a kilogram. The distance the bullet travels through the barrel is 45.0 cm, which is equivalent to 0.45 m.
02

Determine the Acceleration

Use the kinematic equation for acceleration given the initial velocity (\(v_i = 0\), since the bullet starts from rest), final velocity (\(v_f = 965 \text{ m/s}\)), and displacement (\(d = 0.45 \text{ m}\)):\[v_f^2 = v_i^2 + 2ad\]Substitute the known values to solve for acceleration \(a\):\[a = \frac{v_f^2}{2d} = \frac{965^2}{2 \times 0.45}\]Calculate the acceleration.
03

Calculate the Force

With the mass \(m = 0.00420\text{ kg}\) and the calculated acceleration \(a\) from Step 2, apply Newton's second law \(F = ma\) to find the force exerted by the rifle:\[F = 0.00420 \times a\]Insert the value of \(a\) from Step 2 and calculate \(F\).
04

Calculate the Acceleration in Terms of g's

To find the bullet's acceleration in terms of \(g\), divide the calculated acceleration by the standard acceleration due to gravity (\(g = 9.81 \text{ m/s}^2\)):\[a_{in\,g's} = \frac{a}{9.81}\]
05

Calculate the Time in the Barrel

Use the kinematic equation to find the time \(t\) the bullet is in the barrel:\[v_f = v_i + at\]Solve for \(t\):\[t = \frac{v_f - v_i}{a} = \frac{965 - 0}{a}\]Insert the acceleration \(a\) calculated in Step 2 and solve for \(t\).
06

Draw the Free Body Diagram

For part (b), a free-body diagram while in the barrel should show a single force acting horizontally (force applied by the rifle), and vertically the weight of the bullet acting downwards due to gravity. After leaving the barrel, the force acting horizontally is zero because no force acts on the bullet once it exits, only the force due to gravity remains.

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Key Concepts

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

Understanding Kinematics
Kinematics is a branch of physics that focuses on the motion of objects without considering the forces that cause this motion. In this exercise, we are concerned with how far and how fast the bullet moves as it travels through the barrel of the rifle. Since the bullet starts from rest, its initial velocity (\(v_i\)) is zero. It then reaches a final velocity (\(v_f\)) of 965 m/s over a distance (\(d\)) of 0.45 m. The kinematic equations, such as \(v_f^2 = v_i^2 + 2ad\), are used to link these variables with acceleration (\(a\)). By having the initial and final velocity along with the displacement, we calculate the constant acceleration that the bullet undergoes within the barrel. Understanding kinematics is crucial as it forms the backbone of analyzing motions without worrying about the forces yet.
Drawing Free-Body Diagrams
Free-body diagrams are simple diagrams used to show the relative magnitude and direction of all forces acting upon an object. In our exercise, we need to draw two free-body diagrams for the bullet. The first diagram is when the bullet is still within the barrel. At this point, the forces acting on the bullet include:
  • The horizontal force exerted by the rifle on the bullet.
  • The downward gravitational force due to its weight, \(mg\), where \(m\) is mass and \(g\) is acceleration due to gravity.
After the bullet exits the barrel, in the second diagram, no horizontal forces remain since the bullet continues in motion due to the inertia imparted from the force while in the barrel. However, gravity still acts downward on it. These diagrams help in visualizing and solving problems involving forces.
Understanding Constant Acceleration
In the context of the problem, constant acceleration means the bullet gains velocity at a steady rate while traveling through the rifle barrel. This simplification allows us to use kinematic equations directly. The acceleration can be calculated using the equation:\[a = \frac{v_f^2 - v_i^2}{2d}\]. Here, \(v_f\) is the given muzzle velocity, and \(d\) is the distance traveled. With constant acceleration, it’s possible to predict other variables like the time it takes the bullet to exit the barrel, by rearranging the kinematic equation \(v_f = v_i + at\) to solve for time \(t\). This concept is pivotal in problems involving motion under uniform acceleration, providing a straightforward means of calculating various parameters of the motion.
The Art of Conversion of Units
Conversion of units is a fundamental skill in physics that ensures calculations align with consistent units, typically the International System of Units (SI). This exercise involves converting grams to kilograms, and centimeters to meters, since it's crucial to use standard SI units in calculations to avoid errors. For example:
  • Mass: 4.20 g is converted to 0.00420 kg by dividing by 1000 because 1 kilogram equals 1000 grams.
  • Distance: 45.0 cm is converted to 0.45 m by dividing by 100 because 1 meter equals 100 centimeters.
Unit conversion is especially important when using formulas like Newton's second law (\(F = ma\)) or when substituting into kinematic equations, as using inconsistent units can lead to incorrect results.

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Most popular questions from this chapter

A scientific instrument that weighs 85.2 \(\mathrm{N}\) on the earth weighs 32.2 \(\mathrm{N}\) at the surface of Mercury. (a) What is the acceleration due to gravity on Mercury? (b) What is the instrument's mass on earth and on Mercury?

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