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Determine the amplitude of vertical vibration of the car as it travels at a velocity \(v=40 \mathrm{km} / \mathrm{h}\) over the wavy road whose contour may be expressed as a sine or cosine function with a double amplitude \(2 b=50 \mathrm{mm} .\) The mass of the car is \(1800 \mathrm{kg}\) and the stiffness of each of the four car springs is \(35 \mathrm{kN} / \mathrm{m}\) Assume that all four wheels are in continuous con- tact with the road, and neglect damping. Note that the wheelbase of the car and the spatial period of the road are the same at \(L=3 \mathrm{m},\) so that it may be assumed that the car translates but does not rotate. At what critical speed \(v_{c}\) is the vertical vibration of the car at its maximum?

Short Answer

Expert verified
The amplitude of vertical vibration is 25 mm at maximum speed of 37.91 km/h.

Step by step solution

01

Converting Velocity to Meters per Second

Given the velocity is 40 km/h, first convert this to meters per second. Use the conversion factor: 1 km/h = 1000/3600 m/s. Thus, \[ v = 40 \times \frac{1000}{3600} = \frac{1000}{90} \approx 11.11 \text{ m/s} \].
02

Determine Frequency of Road Profile

The road profile is given as a sine or cosine function with a spatial period \(L = 3 \text{ m}\). The wave number \(k\) is given by \(k = \frac{2\pi}{L}\), so \[ k = \frac{2\pi}{3} \text{ rad/m}\]. The frequency of road disturbances \(f_r\) is then given by \[ f_r = \frac{v}{L} = \frac{11.11}{3} \approx 3.70 \text{ Hz}\].
03

Calculate the Resonant Frequency of the Car

The vertical vibration system can be modeled as a single-degree-of-freedom system, where the stiffness per wheel is \(35 \text{ kN/m}\) and there are four wheels. Thus, the total stiffness \(k = 4 \times 35 \times 10^3 \text{ N/m} = 140,000 \text{ N/m}\). The natural frequency \(f_n\) is given by \[ f_n = \frac{1}{2\pi} \sqrt{\frac{k}{m}} = \frac{1}{2\pi} \sqrt{\frac{140,000}{1800}} \approx 3.51 \text{ Hz}\].
04

Determine the Critical Speed for Maximum Amplitude

The vertical vibration amplitude of the car is at its maximum when the frequency of road disturbances \(f_r\) equals the car's natural frequency \(f_n\), i.e., \(f_r = f_n\).Since we have already computed: - \(f_n \approx 3.51 \text{ Hz}\)- \(f_r = \frac{v_c}{L}\)Setting \(f_r = f_n\), we solve for the critical speed \(v_c\):\[ v_c = L \times f_n = 3 \times 3.51 = 10.53 \text{ m/s}\].Convert this back to km/h:\[ v_c = 10.53 \times \frac{3600}{1000} = 37.91 \text{ km/h}\].
05

Calculate the Amplitude of Vertical Vibration

The amplitude of vertical vibration at resonance can be estimated as the amplitude of the road contour because damping is neglected. Given the double amplitude of the road contour is 50 mm, the amplitude of the road oscillation \(b\) is\[ b = \frac{50}{2} = 25 \text{ mm}\].Therefore, the amplitude of the car's vertical vibration \(A\) is approximately \(25 \text{ mm}\) at maximum.

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Key Concepts

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

Natural Frequency
In vibration analysis, the natural frequency of a system is a key concept that describes the rate at which a system oscillates when not subjected to a continuous or repeated external force. Imagine pushing a swing; letting go, the swing moves back and forth at its own natural frequency. For the car in the exercise, its suspension system can be modeled as a spring-mass system. The natural frequency \( f_n \) is determined by the stiffness of the springs and the mass of the car. It can be calculated using the formula: \[ f_n = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]where \( k \) is the stiffness and \( m \) is the mass. Understanding the natural frequency is crucial because it helps predict how the system will behave under different conditions and can be used to design systems that avoid undesirable vibrations.
Identifying the natural frequency helps us know when resonance might occur, which can lead to increased amplitudes of vibration that could damage the vehicle or make the ride uncomfortable.
Resonance
Resonance occurs when the frequency of external vibrations matches the system's natural frequency, leading to a significant increase in the amplitude of oscillations. This can be both beneficial and detrimental, depending on the context. For the car in the exercise, resonance happens when the frequency of the road disturbances equals the car’s natural frequency. At this point, even small vibrations from the road can lead to large vertical vibrations of the car.
In engineering, it's essential to understand and control resonance. For instance, bridges and buildings are designed to avoid resonance with environmental forces like wind or earthquakes. In the automobile context, resonance at certain speeds can cause discomfort or even structural damage, so it must be managed to ensure safety and comfort.
Amplitude of Vibration
The amplitude of vibration refers to the maximum extent of oscillation from the mean position. In simpler terms, it's how high or low the car bounces while driving over the undulating road. In this exercise, the amplitude of vibration of the car at resonance can be estimated to be the same as the amplitude of the road's contour, given that the damping is neglected.
Amplitude is measured in millimeters or meters and directly affects the comfort of the ride. A higher amplitude can make a ride feel bumpier, while a smaller amplitude indicates a smoother experience. In our example, the amplitude of the car’s vertical vibration is approximately 25 mm, which correlates directly with the road's contour amplitude at the resonance speed.
Single-Degree-of-Freedom System
A single-degree-of-freedom (SDOF) system is a simplified model used in vibration analysis to describe systems that can move in only one way, typically linear motion in one direction. The car's suspension system can be modeled as an SDOF system because its vertical motion is constrained by the springs.
Using an SDOF system model simplifies the analysis by reducing the complexities involved in more detailed models. It allows engineers to focus on critical parameters such as mass, stiffness, and damping (if present) and to predict how the system will react to external forces. In this exercise, by viewing the car as an SDOF system, we can more easily calculate its natural frequency and predict under what conditions it might hit resonance.

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Most popular questions from this chapter

A device to produce vibrations consists of the two counter-rotating wheels, each carrying an eccentric mass \(m_{0}=1 \mathrm{kg}\) with a center of mass at a distance \(e=12 \mathrm{mm}\) from its axis of rotation. The wheels are synchronized so that the vertical positions of the unbalanced masses are always identical. The total mass of the device is 10 kg. Determine the two possible values of the equivalent spring constant \(k\) for the mounting which will permit the amplitude of the periodic force transmitted to the fixed mounting to be \(1500 \mathrm{N}\) due to the imbalance of the rotors at a speed of 1800 rev/min. Neglect damping.

A spring-mounted machine with a mass of \(24 \mathrm{kg}\) is observed to vibrate harmonically in the vertical direction with an amplitude of \(0.30 \mathrm{mm}\) under the action of a vertical force which varies harmonically between \(F_{0}\) and \(-F_{0}\) with a frequency of \(4 \mathrm{Hz}\) Damping is negligible. If a static force of magnitude \(F_{0}\) causes a deflection of \(0.60 \mathrm{mm},\) calculate the equivalent spring constant \(k\) for the springs which support the machine.

The equilibrium position of the mass \(m\) occurs where \(y=0\) and \(y_{B}=0 .\) When the attachment \(B\) is given a steady vertical motion \(y_{B}=b \sin \omega t,\) the mass \(m\) will acquire a steady vertical oscillation. Derive the differential equation of motion for \(m\) and specify the circular frequency \(\omega_{c}\) for which the oscillations of \(m\) tend to become excessively large. The stiffness of the spring is \(k\), and the mass and friction of the pulley are negligible.

The spoked wheel of radius \(r,\) mass \(m,\) and centroidal radius of gyration \(\bar{k}\) rolls without slipping on the incline. Determine the natural frequency of oscillation and explore the limiting cases of \(\bar{k}=0\) and \(\bar{k}=r\)

The seismic instrument shown is secured to a ship's deck near the stern where propeller-induced vibration is most pronounced. The ship has a single three-bladed propeller which turns at 180 rev/ \(\min\) and operates partly out of water, thus causing a shock as each blade breaks the surface. The damping ratio of the instrument is \(\zeta=0.5,\) and its undamped natural frequency is \(3 \mathrm{Hz}\). If the measured amplitude of \(A\) relative to its frame is \(0.75 \mathrm{mm},\) compute the amplitude \(\delta_{0}\) of the vertical vibration of the deck.

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