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Four passengers with combined mass \(250 \mathrm{~kg}\) compress the springs of a car with worn-out shock absorbers by \(4.00 \mathrm{~cm}\) when they get in. Model the car and passengers as a single object on a single ideal spring. If the loaded car has a period of vibration of \(1.92 \mathrm{~s}\), what is the period of vibration of the empty car?

Short Answer

Expert verified
The period of vibration of the empty car, computed using the mass of the empty car and the spring constant, gives the final answer.

Step by step solution

01

Calculate the Spring Constant

First, calculate the spring constant using Hooke's Law. The equation is \(F = -kx\), where \(F\) is the force, \(k\) is the spring constant, and \(x\) is the displacement. Here the force \(F\) due to the added passengers is their weight which is their mass times gravity (\(F = mg\)), with \(m = 250 \mathrm{~kg}\) and \(g = 9.8 \mathrm{~m/s^2}\), and the displacement \(x = 0.04 \mathrm{~m}\). So, the spring constant \(k = -F/x\).
02

Calculate the Mass of Car Along with Passengers

Work out the total mass of the car together with the passengers by using the formula for the period of oscillations, rearranging it to solve for \(m\). The formula is \(T = 2\pi (m/k)^{0.5}\), with \(T = 1.92 \mathrm{~s}\), \(k\) from the previous step, and \(m\) being the mass we want to find. Hence, \(m = (T/2\pi)^2 * k \).
03

Determine the Mass of the Empty Car

Find the mass of the empty car by subtracting the mass of the passengers from the total mass found in step 2. As the mass of passengers is given as 250 kg, the mass of the empty car equals \(m_{\text{total}} - 250 \mathrm{~kg}\).
04

Compute the Period of the Empty Car

Calculate the period of vibration of the empty car \(T'\) using the formula from step 2, but this time with the mass of the empty car \(m_{\text{car}}\) and the same spring constant \(k\). Thus, \(T' = 2\pi (m_{\text{car}}/k)^{0.5}\).

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Key Concepts

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

Hooke's Law
Understanding Hooke's Law is fundamental to analyzing the behavior of springs and elastic materials. Simply put, Hooke's Law states that the force needed to extend or compress a spring by some distance is proportional to that distance.

The law is mathematically expressed as \( F = -kx \), where \( F \) represents the force applied on the spring, \( x \) is the distance the spring is stretched or compressed from its original equilibrium position, and \( k \) is a constant characteristic of the spring, known as the spring constant. The negative sign indicates that the force exerted by the spring is in the opposite direction to the displacement.

Let's take an example from our exercise where the car's springs compress due to the weight of the passengers. If the springs are compressed by \( 4.00 \text{cm} \) when the passengers enter the car, then the force exerted by the passengers (their weight) can be set equal to the spring force to find the spring constant \( k \). This relationship is pivotal for determining other dynamic properties of the spring-mass system such as its period of vibration.
Spring Constant
The spring constant, denoted by \( k \), is a measure of a spring's stiffness. It plays a critical role in the dynamics of spring-mass systems. In the context of Hooke's Law, the spring constant relates the force exerted by the spring to the displacement caused in that spring. Specifically, the higher the spring constant, the stiffer the spring, and thus the more force required to compress or extend it by a certain amount.

In our problem involving the car, the spring constant determines how the car will oscillate when it's set in motion, and is calculated through the equation derived from Hooke's Law. By knowing the weight of the passengers and the displacement of the springs, we can determine the spring constant. This constant remains the same regardless of whether the car is empty or loaded, stipulating that the spring's intrinsic property does not change with different loads.
Oscillation
Oscillation occurs when an object experiences a repetitive back-and-forth movement around a central point, or equilibrium position. In the case of the car and its passengers, when the passengers sit inside the car and compress the springs, and then when they depart, allowing the springs to extend back out, a cycle of oscillations could commence.

The period of vibration, which is the time for one complete cycle of oscillation, is of particular interest as it describes the oscillatory motion's tempo. The formula for the period \(T\) of a mass-spring system is given by \( T = 2\pi\sqrt{m/k} \), where \( m \) is the mass of the object attached to the spring and \( k \) is the spring constant. From our exercise solution, we see that if we have the spring constant and the mass of the car (with or without the passengers), we can easily calculate the car's period of vibration.

Understanding these concepts is not only critical for solving physics problems but also for appreciating the principles that govern many mechanical systems in engineering and nature.

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Most popular questions from this chapter

An unhappy \(0.300 \mathrm{~kg}\) rodent, moving on the end of a spring with force constant \(k=2.50 \mathrm{~N} / \mathrm{m},\) is acted on by a damping force \(F_{x}=-b v_{x}\). (a) If the constant \(b\) has the value \(0.900 \mathrm{~kg} / \mathrm{s},\) what is the frequency of oscillation of the rodent? (b) For what value of the constant \(b\) will the motion be critically damped?

A small block is attached to an ideal spring and is moving in SHM on a horizontal, frictionless surface. The amplitude of the motion is \(0.165 \mathrm{~m}\). The maximum speed of the block is \(3.90 \mathrm{~m} / \mathrm{s}\). What is the maximum magnitude of the acceleration of the block?

A block of mass \(m\) is undergoing SHM on a horizontal, friction less surface while attached to a light, horizontal spring. The spring has force constant \(k,\) and the amplitude of the motion of the block is \(A\). (a) The average speed is the total distance traveled by the block divided by the time it takes it to travel this distance. Calculate the average speed for one cycle of the SHM. (b) How does the average speed for one cycle compare to the maximum speed \(v_{\max } ?\) (c) Is the average speed more or less than half the maximum speed? Based on your answer, does the block spend more time while traveling at speeds greater than \(v_{\max } / 2\) or less than \(v_{\max } / 2 ?\)

SHM of a Floating Object. An object with height \(h\)mass \(M\), and a uniform cross-sectional area \(A\) floats upright in a liquid with density \(\rho\). (a) Calculate the vertical distance from the surface of the liquid to the bottom of the floating object at equilibrium. (b) A downward force with magnitude \(F\) is applied to the top of the object. At the new equilibrium position, how much farther below the surface of the liquid is the bottom of the object than it was in part (a)? (Assume that some of the object remains above the surface of the liquid.) (c) Your result in part (b) shows that if the force is suddenly removed, the object will oscillate up and down in SHM. Calculate the period of this motion in terms of the density \(\rho\) of the liquid, the mass \(M,\) and the cross-sectional area \(A\) of the object. You can ignore the damping due to fluid friction (see Section 14.7).

A \(5.00 \mathrm{~kg}\) partridge is suspended from a pear tree by an ideal spring of negligible mass. When the partridge is pulled down \(0.100 \mathrm{~m}\) below its equilibrium position and released, it vibrates with a period of \(4.20 \mathrm{~s}\). (a) What is its speed as it passes through the equilibrium position? (b) What is its acceleration when it is \(0.050 \mathrm{~m}\) above the equilibrium position? (c) When it is moving upward, how much time is required for it to move from a point \(0.050 \mathrm{~m}\) below its equilibrium position to a point \(0.050 \mathrm{~m}\) above it? (d) The motion of the partridge is stopped, and then it is removed from the spring. How much does the spring shorten?

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