A mass-spring system oscillates so that the position of the mass is described by \(x=-10 \cos (1.57 t),\) where \(x\) is in \(\mathrm{cm}\) when \(t\) is in seconds. Make a plot that has a dot for the position of the mass at $t=0, t=0.2 \mathrm{s}, t=0.4 \mathrm{s}, \ldots, t=4 \mathrm{s}$ The time interval between each dot should be 0.2 s. From your plot, tell where the mass is moving fastest and where slowest. How do you know?

Short Answer

Expert verified
Answer: The mass is moving fastest at the peak and trough (extreme positions) of the oscillation and slowest as it passes through the equilibrium position (x = 0).

Step by step solution

01

Understand the equation

The position of the mass is given by the equation \(x=-10 \cos (1.57 t)\). Here, \(x\) represents the position of the mass (in centimeters) and \(t\) represents time (in seconds).
02

Generate data points for the plot

We need data points for the position of the mass at 0.2 second intervals for \(t=0s\) to \(t=4s\). By plugging the values of \(t\) into the equation, we can find the corresponding \(x\) values (position).
03

Calculate position values for the given time intervals

Using the equation \(x=-10 \cos (1.57 t)\), calculate the position of the mass for the required time intervals: t=0: \(x= -10 \cos (1.57 \cdot 0) = -10\) t=0.2: \(x=-10 \cos (1.57 \cdot 0.2) \approx 4.1\) t=0.4: \(x=-10 \cos (1.57 \cdot 0.4) \approx 9.2\) t=0.6: \(x=-10 \cos (1.57 \cdot 0.6) \approx 8.6\) t=0.8: \(x=-10 \cos (1.57 \cdot 0.8) \approx 1.1\) . . . t=4: \(x=-10 \cos (1.57 \cdot 4) \approx -10\)
04

Plot the data points

Using the calculated data points, plot the position of the mass over time with a dot for each time interval.
05

Analyze the plot and determine where the mass is moving fastest and slowest

Examine the plot to determine where the mass is moving the fastest and slowest. The steeper the slope of the line between two points, the faster the mass is moving, while the less steep (or more horizontal) the slope, the slower the mass is moving. From analyzing the plot, we can determine that the mass is moving fastest at the peak and trough (extreme positions) of the oscillation and slowest as it passes through the equilibrium position (x = 0). This is because as the mass moves away from the equilibrium position, the restoring force (spring force) increases, and when it reaches the extreme positions, the restoring force is at its maximum, hence the mass is moving fastest. When the mass is at the equilibrium position, the restoring force is at its minimum, and thus the mass is moving slowest.

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

A clock has a pendulum that performs one full swing every \(1.0 \mathrm{s}(\) back and forth). The object at the end of the pendulum weighs $10.0 \mathrm{N}$. What is the length of the pendulum?
The maximum height of a cylindrical column is limited by the compressive strength of the material; if the compressive stress at the bottom were to exceed the compressive strength of the material, the column would be crushed under its own weight. (a) For a cylindrical column of height \(h\) and radius \(r,\) made of material of density \(\rho,\) calculate the compressive stress at the bottom of the column. (b) since the answer to part (a) is independent of the radius \(r,\) there is an absolute limit to the height of a cylindrical column, regardless of how wide it is. For marble, which has a density of $2.7 \times 10^{3} \mathrm{kg} / \mathrm{m}^{3}\( and a compressive strength of \)2.0 \times 10^{8} \mathrm{Pa},$ find the maximum height of a cylindrical column. (c) Is this limit a practical concern in the construction of marble columns? Might it limit the height of a beanstalk?
An empty cart, tied between two ideal springs, oscillates with $\omega=10.0 \mathrm{rad} / \mathrm{s} .$ A load is placed in the cart. making the total mass 4.0 times what it was before. What is the new value of \(\omega ?\)
A marble column with a cross-sectional area of \(25 \mathrm{cm}^{2}\) supports a load of \(7.0 \times 10^{4} \mathrm{N} .\) The marble has a Young's modulus of \(6.0 \times 10^{10} \mathrm{Pa}\) and a compressive strength of $2.0 \times 10^{8} \mathrm{Pa} .$ (a) What is the stress in the column? (b) What is the strain in the column? (c) If the column is \(2.0 \mathrm{m}\) high, how much is its length changed by supporting the load? (d) What is the maximum weight the column can support?
A wire of length \(5.00 \mathrm{m}\) with a cross-sectional area of $0.100 \mathrm{cm}^{2}\( stretches by \)6.50 \mathrm{mm}\( when a load of \)1.00 \mathrm{kN}$ is hung from it. What is the Young's modulus for this wire?
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