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A weight is tied to the end of a spring and then set into motion. The displacement of the weight from equilibrium is given by the equation \(y=4\left[\frac{\sin \left(2 t-\frac{\pi}{2}\right)+1}{1+\csc \left(2 t-\frac{\pi}{2}\right)}\right]\), where \(t\) is time in seconds. Simplify the equation and then describe the maximum displacement with respect to the equilibrium position, and how long it takes for the weight to first achieve its maximum starting at \(t=0\).

Short Answer

Expert verified
The maximum displacement is 4 units and occurs at approximately 0.785 seconds after starting at \(t=0\).

Step by step solution

01

Understand the function

The equation given is \(y=4\left[\frac{\sin \left(2 t-\frac{\pi}{2}\right)+1}{1+\csc \left(2 t-\frac{\pi}{2}\right)}\right]\). This is a trigonometric function representing the displacement of the weight over time.
02

Simplify the equation

Recognize that \(\csc(x) = \frac{1}{\sin(x)}\). Rewrite \(1 + \csc\left(2t - \frac{\pi}{2}\right)\) as \(1 + \frac{1}{\sin(2t - \frac{\pi}{2})}\), then simplify: \[1 + \frac{1}{\sin(2t - \frac{\pi}{2})} = \frac{\sin(2t - \frac{\pi}{2}) + 1}{\sin(2t - \frac{\pi}{2})}\]. Now substitute back into the original equation: \(y = 4\left[\frac{\sin(2t - \frac{\pi}{2}) + 1}{\frac{\sin(2t - \frac{\pi}{2}) + 1}{\sin(2t - \frac{\pi}{2})}}\right] = 4 \sin(2t - \frac{\pi}{2})\).
03

Analyze the simplified equation

The simplified equation \(y = 4 \sin(2t - \frac{\pi}{2})\) is a sine wave with amplitude 4. The positive maximum value of \(\sin(x)\) is 1, causing the function to reach a maximum displacement of 4 units from equilibrium.
04

Determine when the maximum displacement occurs

A sine function reaches its maximum at \((2n+1)\frac{\pi}{2}\), where \(n\) is an integer. For \(2t - \frac{\pi}{2} = \frac{\pi}{2}\), solve for \(t\): \(2t = \pi\), giving \(t = \frac{\pi}{2} \cdot \frac{1}{2} = \frac{\pi}{4} \approx 0.785\) seconds.

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Key Concepts

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

spring motion
In the world of physics, a spring motion is an excellent demonstration of harmonic motion. This happens when a weight attached to a spring bounces up and down over time. The weight moves in such a way that it regularly returns to a stable position called the equilibrium. This situation, known as simple harmonic motion, can be described using trigonometric functions. In this particular scenario, our equation models the up-and-down movement of the weight at the end of the spring. The displacement of the weight is calculated using the trigonometric function given in the problem. By understanding this, students can gain insight into more complex physics topics, like oscillations and wave phenomena.
  • Harmonic motion is periodic, meaning it repeats itself in a regular cycle.
  • The equilibrium position is where the net force on the weight is zero.

Spring motion equations help in identifying how forces affect moving objects. By analyzing these equations, you can understand the motion details, like amplitude and phase shifting.
sine function
The sine function is a key player in depicting periodic changes, like those seen in spring motion. This mathematical function is used because it smoothly cycles between -1 and 1, modeling the oscillating behavior perfectly. The equation simplifies to a sine function, showing how it controls the motion with its continuous waves.

Key properties of a sine function include:
  • Amplitude - This is the height from the center line to the peak of the wave. In the simplified equation, it's 4, meaning the maximum height of the displacement wave is 4 units.
  • Phase Shift - Given by \(2t - \frac{\pi}{2}\), it determines how the function is shifted horizontally.

With a sine function like \(4 \sin(2t - \frac{\pi}{2})\), the periodic nature ensures that the weight's displacement from equilibrium follows a consistent and predictable wave. This understanding is crucial in solving problems related to oscillatory motion in physics.
maximum displacement
When we talk about maximum displacement, we refer to the farthest point the weight moves from its equilibrium position. This peak occurs when the sine function reaches its maximum value, which is 1.
This means that for our equation \(y = 4 \sin(2t - \frac{\pi}{2})\), the maximum displacement is 4 units.

To determine when this occurs, you need to find when the sine function itself equals 1. This happens at specific points, namely every half pi radians. The first of these occurs at \(2t - \frac{\pi}{2} = \frac{\pi}{2}\). Solving this for \(t\), we find \(t = \frac{\pi}{4} \approx 0.785\) seconds. This is the first instance the weight reaches its maximum displacement.
  • This timing is crucial in applications like designing springs for mechanical systems.
  • Understanding maximum displacement helps in evaluating the efficiency and capacity of oscillating systems.

Grasping these concepts allows you to predict and manage the movement of systems subject to harmonic motion.

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Most popular questions from this chapter

For Exercises 69-72, refer to the following: One cannot prove that an equation is an identity using technology, but one can use it as a first step to see whether the equation seems to be an identity. Using a graphing calculator, plot \(Y_{1}=\left(\frac{x}{2}\right)-\frac{\left(\frac{x}{2}\right)^{3}}{3 !}+\frac{\left(\frac{x}{2}\right)^{5}}{5 !}\) and \(Y_{2}=\sin \left(\frac{x}{2}\right)\) for \(x\) range \([-1,1]\). Is \(Y_{1}\) a good approximation to \(Y_{2}\) ?

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For Exercises 55 and 56, refer to the following: Monthly profits can be expressed as a function of sales, that is, \(p(s)\). A financial analysis of a company has determined that the sales \(s\) in thousands of dollars are also related to monthly profits \(p\) in thousands of dollars by the relationship: $$ \tan \theta=\frac{p}{s} \text { for } 0 \leq s \leq 50,0 \leq p<40 $$ Based on sales and profits, it can be determined that the domain for angle \(\theta\) is \(0 \leq \theta \leq 38^{\circ}\). If monthly profits are $$\$ 3000$$ and monthly sales are $$\$ 4000$$, find \(\tan \left(\frac{\theta}{2}\right)\).

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