A vehicle of mass \(m\), with suspension of stiffness \(k\) and negligible damping, is traveling at constant speed \(v_{0}\) when it encounters the series of equally spaced semi-circular speed bumps shown. Assuming that no slip occurs between the wheel and the road, determine (a) the motion of the engine block while it is traveling over this part of the roadway and \((b)\) the force transmitted to the block.

Short Answer

Expert verified
Answer: The motion of the engine block can be described as a function of time using the harmonic motion equation: y(t) = A * cos(ωt), where A is the amplitude of the motion and ω is the angular frequency. The force transmitted to the engine block is determined using Newton's second law, F(t) = m * a(t), where a(t) is the acceleration found by taking the second derivative of the displacement y(t).

Step by step solution

01

Determine the angular frequency ω

When the vehicle encounters the speed bumps, it oscillates back and forth over the bumps, creating a sinusoidal pattern in its motion. The angular frequency ω is the rate at which the vehicle oscillates. As the vehicle moves forward at a constant speed v0, the bump frequency f can be determined by dividing the speed v0 by the distance between the bumps L, such that f = v0/L. We can find the angular frequency ω using the equation ω = 2πf.
02

Determine the amplitude A of the motion

The amplitude A of the motion is the maximum displacement of the vehicle from its equilibrium position. This can be found using the equation A = R, where R is the radius of the semi-circular bumps. Since the vehicle moves over semi-circular speed bumps, the radius R is equal to half the distance between the peaks of the bumps.
03

Calculate the motion of the engine block (a)

To determine the motion of the engine block, we will analyze its vertical displacement y(t) as a function of time. For this, we will use the following equation for harmonic motion: y(t) = A * cos(ωt). Since we have already found the amplitude A and angular frequency ω in previous steps 1 and 2, we can substitute them into the equation to determine the motion of the engine block as a function of time.
04

Calculate the force transmitted to the engine block (b)

To find the force transmitted to the engine block, we will first determine the acceleration a(t) of the vehicle, which can be found using the second derivative of the displacement y(t) that we calculated in step 3. The acceleration equation is a(t) = -ω^2 * A * cos(ωt). Next, we will use Newton's second law F = ma to find the force transmitted to the engine block. By substituting the mass m and the acceleration a(t) into the equation, we can determine the force F(t). Following these steps will help you find the motion of the engine block and the force transmitted to it as the vehicle travels over the series of semi-circular speed bumps.

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!

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

The damping factor for a shaft-turbine system is measured to be \(0.15\). When the turbine rotates at a rate equal to \(120 \%\) of the undamped natural frequency of the shaft, the system is observed to whirl with an amplitude equal to the radius of the shaft. What will be the amplitude of whirling when the rotation rate of the turbine is reduced to \(80 \%\) of the undamped natural frequency of the shaft if the radius of the shaft is 1 inch?

An aircraft mock-up for ground testing is modeled as shown, where a brace represented as a torsional spring of stiffness \(k_{T}\) has been attached at the pivot support to restrain excessive yawing. It is assumed that during a test, both thrusters will exert a constant force of magnitude \(F_{0}\). However, during a simulation, one of the thrusters deviates from the prescribed force by adding a perturbation in the form of a harmonic thrust of small amplitude. Thus, the force applied by this thruster takes the form \(F(t)=F_{0}(1+\varepsilon \sin \Omega t)\), as indicated, where \(\varepsilon \ll 1\). Determine the steady state yawing motion of the mock-up. What is the amplitude of the response at resonance?

A horizontally directed harmonic force \(F(t)=F_{0} \sin \Omega t\) acts on the bob of mass \(m\) of a simple pendulum of length \(L\). Determine the steady state response of the pendulum.

Several bolts on the propeller of a fanboat detach, resulting in an offset moment of \(5 \mathrm{lb}-\mathrm{ft}\). Determine the amplitude of bobbing of the boat when the fan rotates at \(200 \mathrm{rpm}\), if the total weight of the boat and passengers is \(1000 \mathrm{lb}\) and the wet area projection is approximately \(30 \mathrm{sq} \mathrm{ft}\). What is the amplitude at $1000 \mathrm{rpm}$ ?

A 3000 pound cylindrical pontoon having a radius of 6 feet floats in a body of fluid. A driver exerts a harmonic force of magnitude \(500 \mathrm{lb}\) at a rate of \(200 \mathrm{cy}-\) cles per minute at the center of the up- per surface of the float as indicated. \((a)\) Determine the density of the fluid if the pontoon is observed to bob with an amplitude of 1 foot. (b) What is the magnitude of the bobbing motion of the pontoon when the excitation fre- quency is reduced to \(5 \mathrm{rad} / \mathrm{sec}\) ?

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