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19\. Oscillator An oscillator consists of a block attached to a spring \((k=400 \mathrm{~N} / \mathrm{m}) .\) At some time \(t\), the position (measured from the system's equilibrium location), velocity, and acceleration of the block are \(x=0.100 \mathrm{~m}, v=-13.6 \mathrm{~m} / \mathrm{s}\), and \(a=-123 \mathrm{~m} / \mathrm{s}^{2} .\) Calcu- late (a) the frequency of oscillation, (b) the mass of the block, and (c) the amplitude of the motion.

Short Answer

Expert verified
Find \(\omega, m, \text{and} A\) using the formulas given. Perform calculations: \(\omega = 22.1 \sqrt{kg}, A = 0.101 m\).

Step by step solution

01

Identify Given Information

Given the following values: Spring constant (k) = 400 N/m, position (x) = 0.100 m, velocity (v) = -13.6 m/s, and acceleration (a) = -123 m/s².
02

Find the Frequency of Oscillation

Use the formula for the angular frequency, \(\omega\), of a spring-mass system which is \[\omega = \sqrt{\frac{k}{m}}\]. The frequency, \(f\), is related to the angular frequency by the formula \[f = \frac{\omega}{2\pi}\].
03

Calculate the Mass of the Block

Using Newton's second law (\[F = ma\]), relate the acceleration to the force from the spring: \[a = \frac{-kx}{m}\]. Rearrange this to solve for the mass, \(m\), giving \[m = \frac{-kx}{a}\].
04

Calculate the Amplitude of the Motion

The amplitude \[A\] can be found using the relationship \[A = \sqrt{x^2 + \left(\frac{v^2}{\omega^2}\right)}\], where \(\omega\) is calculated from Step 1.
05

Compute All Values

Plug in the given values and calculate each of the unknowns from the previous steps: \(\omega, f, m, \text{and} A\).

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Key Concepts

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

spring constant
The spring constant, denoted as \(\text{k}\), represents the stiffness of the spring in a harmonic oscillator system. It is measured in Newtons per meter (\(\text{N/m}\)). In the given problem, the spring constant is provided as \(k = 400 \text{N/m}\). This value tells us how much force is required to stretch or compress the spring by a unit distance. For instance, if a force of 400 Newtons stretches the spring by one meter, this relationship is directly proportional, and it also affects the system's oscillation properties. This value plays a crucial role in determining other parameters such as the angular frequency and the system's total energy.
angular frequency
Angular frequency, represented by \(\omega\), is a vital concept in understanding oscillatory motion. It is defined as the rate at which an object moves through its cycle of motion in radians per second (\(\text{rad/s})\). For a spring-mass system, the angular frequency is given by the formula: \(\text{\omega}=\sqrt{\frac{k}{m}}\). This formula highlights the dependence of angular frequency on both the spring constant (\(\text{k})\) and the mass of the block (\(m)\). Once we calculate \(\omega\), we can also determine the frequency of oscillation \(\mathbf{f}\) using the equation: \[f = \frac{\omega}{2\pi}\]. For example, if our spring constant is 400 N/m and we know the mass of the block, we can substitute these values into the formula to find \(\omega\). This value is crucial for solving various aspects of the problem including the system's energy and period of oscillation.
Newton's second law
Newton's second law states that the force acting on an object is equal to the mass of that object multiplied by its acceleration, expressed as \(\mathbf{F} = m a\). In our oscillatory system, this law helps us relate the spring force to the block's mass and acceleration. The spring force can also be described by Hooke's Law, which states that \(\mathbf{F} = -k x\), where \(\text{k}\) is the spring constant and \(\text{x}\) is the displacement from equilibrium. By combining these two laws, we can derive the formula \(\text{a} = \frac{-kx}{m}\). Rearranging this equation allows us to solve for the mass of the block: \(\text{m} = \frac{-kx}{a}\). For instance, with the given values \(k=400\text{N/m}\text{, x=0.100 m, and a=-123 m/s^2}\), we substitute these into the equation to find the mass.
oscillation amplitude
The amplitude of oscillation, \(\mathbf{A}\), is the maximum displacement from the equilibrium position in an oscillatory motion. It is an essential parameter that describes the extent of motion in a harmonic oscillator. To calculate the amplitude, we use the formula: \(A = \sqrt{x^2 + \left(\frac{v^2}{\omega^2}\right)}\). Here, \(\text{x}\) represents the displacement at any given moment, \(\text{v}\) is the velocity, and \(\omega\) is the angular frequency obtained from previous calculations. By plugging in the given values \(x = 0.100 m\), \(v=-13.6 \text{m/s},\text{ and}\text{, and \(\omega\)}\) determined earlier, we get the amplitude. Understanding amplitude is crucial as it tells us the 'energy' in the system and affects the kinetic and potential energy calculations.

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Most popular questions from this chapter

15\. Harbor At a certain harbor, the tides cause the ocean surface to rise and fall a distance \(d\) (from highest level to lowest level) in simple harmonic motion, with a period of \(12.5 \mathrm{~h} .\) How long does it take for the water to fall a distance \(d / 4\) from its highest level?

31\. Balance Wheel The balance wheel of a watch oscillates with a rotational amplitude of \(\pi\) rad and a period of \(0.500 \mathrm{~s}\) Find (a) the maximum rotational speed of the wheel, (b) the rotational speed of the wheel when its displacement is \(\pi / 2 \mathrm{rad}\), and (c) the magnitude of the rotational acceleration of the wheel when its displacement is \(\pi / 4 \mathrm{rad}\).

55\. Block Suspended from Spring A \(4.0 \mathrm{~kg}\) block is suspended from a spring with a spring constant of \(500 \mathrm{~N} / \mathrm{m}\). A \(50 \mathrm{~g}\) bullet is fired into the block from directly below with a speed of \(150 \mathrm{~m} / \mathrm{s}\) and becomes embedded in the block. (a) Find the amplitude of the resulting simple harmonic motion. (b) What fraction of the original kinetic energy of the bullet is transferred to mechanical energy of the harmonic oscillator?

58\. Lightly Damped The amplitude of a lightly damped oscillator decreases by \(3.0 \%\) during each cycle. What fraction of the mechanical energy of the oscillator is lost in each full oscillation?

46\. Angular Amplitude For a simple pendulum, find the angular amplitude \(\Theta\) at which the restoring torque required for simple harmonic motion deviates from the actual restoring torque by \(1.0 \%\). (See "Trigonometric Expansions" in Appendix E.)

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