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A mass \(m=5.00 \mathrm{~kg}\) is suspended from a spring and oscillates according to the equation of motion \(x(t)=0.5 \cos (5 t+\pi / 4) .\) What is the spring constant?

Short Answer

Expert verified
Answer: The spring constant for the system is 125 N/m.

Step by step solution

01

Identify the equation of motion parameters

In this problem, we are given the equation of motion as \(x(t) = 0.5 \cos (5 t + \pi/4)\). This is the equation for simple harmonic motion in the form of \(x(t) = A \cos (\omega t + \phi)\), where \(A\) is the amplitude, \(\omega\) is the angular frequency, and \(\phi\) is the phase angle. By comparing the given equation, we can identify the following parameters: Amplitude (A): \(0.5 \mathrm{~m}\) Angular Frequency (\(\omega\)): \(5 \mathrm{~s^{-1}}\) Phase Angle (\(\phi\)): \(\pi/4 \mathrm{~rad}\)
02

Calculate the frequency and the period

Next, we will find the frequency (f) and the period (T) of the oscillation, since they will be useful in determining the spring constant. We can use the following relationships between angular frequency, frequency, and period: \(\omega = 2 \pi f\) and \(T = \dfrac{1}{f}\) From the given equation, we have an angular frequency (\(\omega\)) of 5 : \(f = \dfrac{\omega}{2 \pi} = \dfrac{5}{2 \pi} \approx 0.796 \mathrm{~Hz}\) Now we can calculate the period (T): \(T = \dfrac{1}{f} = \dfrac{1}{0.796} \approx 1.256 \mathrm{~s}\)
03

Determine the spring constant using Hooke's Law

To find the spring constant, we will use Hooke's Law and the relationship between the period and mass on a spring: Hooke's Law: \(F = -kx\) Relationship between period and mass: \(T = 2\pi \sqrt{\frac{m}{k}}\) The force acting on the mass due to the spring (F) is the product of mass (m) and acceleration (a). In simple harmonic motion, acceleration is given by \(a = -\omega^{2} x\). Thus, \(F = -ma = m\omega^{2}x\) Substituting Hooke's Law into this equation, we get: \(kx = m\omega^{2}x\) Now, we will solve for the spring constant (k). Since x 鈮 0, we can divide both sides by x: \(k = m\omega^{2}\) Finally, we will plug in the given mass (m = 5.00 kg) and the angular frequency (\(\omega\) = 5 s鈦宦): \(k = (5.00 \mathrm{~kg}) (5 \mathrm{~s^{-1}})^{2} = 5 \cdot 25 = 125 \mathrm{~N/m}\) The spring constant is 125 N/m.

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Key Concepts

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

Simple Harmonic Motion
Simple Harmonic Motion (SHM) is a type of periodic motion, like the swing of a pendulum or the vibration of a guitar string, where the restoring force is directly proportional to the displacement and acts in the opposite direction. It's characterized by oscillations about an equilibrium position. The motion is 'simple' because it can be described by simple equations and 'harmonic' because it is periodic and follows a harmonic function, typically sinusoidal. In the given exercise, a mass attached to a spring demonstrates SHM as it moves back and forth, where the displacement from the equilibrium position follows a cosine function of time.
Hooke's Law
Hooke's Law is a principle that states the force required to extend or compress a spring by some distance (x) is proportional to that distance. Mathematically, it can be expressed as:

\(F = -kx\)

Here, \(F\) is the force applied, \(k\) is the spring constant, and \(x\) is the displacement from the original length of the spring. The negative sign indicates that the force exerted by the spring opposes the displacement. This law is crucial in determining the behavior of the spring and the motion of the mass attached to it. In the context of the exercise, Hooke's Law is instrumental in finding the spring constant by relating force to displacement.
Angular Frequency
Angular frequency (\(\omega\)) is a measure of how fast something is oscillating in SHM and is related to the number of oscillations an object completes in a unit of time (frequency). It's represented in radians per second and is given by the equation:

\(\omega = 2\pi f\)

where \(f\) is the frequency in cycles per second, or Hertz (Hz), and \(2\pi\) is the factor needed to convert frequency to angular frequency (since there are \(2\pi\) radians in a full cycle). Angular frequency is crucial to understanding the timing of the oscillations, which in turn helps in calculating other important quantities like the spring constant.
Oscillation Equation
The oscillation equation in the context of SHM provides a way to calculate the position of the oscillating object at any given time (t), which is particularly helpful in applications like the design of springs and pendulums. It can be represented as:

\(x(t) = A \cos (\omega t + \phi)\)

In this equation, \(A\) represents the amplitude, \(\omega\) is the angular frequency, \(\phi\) is the phase constant determining the initial angle, and \(t\) is the time variable. This equation gives us a full description of the motion of the object in time, and in the exercise, it allowed us to determine the mass's motion on the spring to find the spring constant.

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Most popular questions from this chapter

Two pendulums of identical length of \(1.000 \mathrm{~m}\) are suspended from the ceiling and begin swinging at the same time. One is at Manila, in the Philippines, where \(g=9.784 \mathrm{~m} / \mathrm{s}^{2}\) and the other is at Oslo, Norway, where \(g=9.819 \mathrm{~m} / \mathrm{s}^{2},\) After how many oscillations of the Manila pendulum will the two pendulums be in phase again? How long will it take for them to be in phase again?

Mass-spring systems and pendulum systems can both be used in mechanical timing devices. What are the advantages of using one type of system rather than the othes in a device designed to generate reproducible time measurements over an extended period of time?

A Foucault pendulum displayed in a museum is typically quite long, making the effect easier to see. Consider a Foucault pendulum of length \(15 \mathrm{~m}\) with a 110 -kg brass bob. It is set to swing with an amplitude of \(3.5^{\circ}\) a) What is the period of the pendulum? b) What is the maximum kinetic energy of the pendulum? c) What is the maximum speed of the pendulum?

The motion of a planet in a circular orbit about a star obeys the equations of simple harmonic motion. If the orbit is observed edge-on, so the planet's motion appears to be onedimensional, the analogy is quite direct: The motion of the planet looks just like the motion of an object on a spring a) Use Kepler's Third Law of planetary motion to determine the "spring constant" for a planet in circular orbit around a star with period \(T\) b) When the planet is at the extremes of its motion observed edge-on, the analogous "spring" is extended to its largest displacement. Using the "spring" analogy, determine the orbital velocity of the planet.

A spring is hanging from the ceiling with a mass attached to it. The mass is pulled downward, causing it to oscillate vertically with simple harmonic motion. Which of the following will increase the frequency of oscillation? a) adding a second, identical spring with one end attached to the mass and the other to the ceiling b) adding a second, identical spring with one end attached to the mass and the other to the floor c) increasing the mass d) adding both springs, as described in (a) and (b)

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