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When a 0.750-kg mass oscillates on an ideal spring, the frequency is 1.75 Hz. What will the frequency be if 0.220 kg are (a) added to the original mass and (b) subtracted from the original mass? Try to solve this problem \(without\) finding the force constant of the spring.

Short Answer

Expert verified
New frequency is 1.55 Hz when mass is added, and 2.10 Hz when mass is subtracted.

Step by step solution

01

Understanding the problem

We have a 0.750 kg mass attached to an ideal spring with an oscillation frequency of 1.75 Hz. We need to calculate the new frequencies when 0.220 kg is added and when 0.220 kg is subtracted from the original mass.
02

Recall the formula for frequency of oscillation

The frequency of a mass-spring system is given by the formula: \[ f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]where \( f \) is the frequency, \( k \) is the spring constant, and \( m \) is the mass.
03

Express the initial frequency

Given the initial mass \( m_1 = 0.750 \) kg and frequency \( f_1 = 1.75 \) Hz, we use: \[ f_1 = \frac{1}{2\pi} \sqrt{\frac{k}{m_1}} \]Solving for the spring constant, we don't need its value, but note how it scales: \[ f_1^2 = \frac{k}{4\pi^2 m_1} \]
04

Calculate new frequency when additional mass is added

New mass \( m_2 = 0.750 + 0.220 = 0.970 \) kg. The new frequency \( f_2 \) is:\[ f_2 = \frac{1}{2\pi} \sqrt{\frac{k}{m_2}} \]Using the relationship, \( f_2^2 = \frac{k}{4\pi^2 m_2} \). Therefore,\[ \frac{f_2}{f_1} = \sqrt{\frac{m_1}{m_2}} \]\[ f_2 = f_1 \times \sqrt{\frac{m_1}{m_2}} \]\[ f_2 = 1.75 \times \sqrt{\frac{0.750}{0.970}} \approx 1.55 \text{ Hz} \]
05

Calculate new frequency when mass is subtracted

New mass \( m_3 = 0.750 - 0.220 = 0.530 \) kg. The new frequency \( f_3 \) is: \[ f_3 = \frac{1}{2\pi} \sqrt{\frac{k}{m_3}} \]Using our relationship, \( f_3^2 = \frac{k}{4\pi^2 m_3} \). Therefore,\[ \frac{f_3}{f_1} = \sqrt{\frac{m_1}{m_3}} \]\[ f_3 = f_1 \times \sqrt{\frac{m_1}{m_3}} \]\[ f_3 = 1.75 \times \sqrt{\frac{0.750}{0.530}} \approx 2.10 \text{ Hz} \]

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Key Concepts

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

Frequency of Oscillation
Let's dig into what frequency of oscillation means, especially in a mass-spring system. Frequency refers to how many times an object vibrates back and forth in one second. It is measured in Hertz (Hz), where 1 Hz equals one complete oscillation or cycle per second. In the context of a mass-spring system, the frequency is determined by both the mass attached to the spring and the spring's stiffness, or spring constant.The essential formula for frequency in such a system is:\[ f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]In this formula:
  • \( f \) stands for frequency.
  • \( k \) is the spring constant, representing the spring's stiffness.
  • \( m \) represents the mass attached to the spring.
Understanding the effect of mass on frequency is crucial. As the mass increases, the frequency decreases. This is because a heavier mass makes the system oscillate slower. Conversely, when the mass decreases, the frequency increases, making the system oscillate faster.So, when additional mass is added to or removed from the system, recalculating the frequency can determine how the oscillation behavior changes.
Mass-Spring System
A mass-spring system is a fundamental concept in physics where a mass (an object with weight) is attached to a spring. This system is significant because it demonstrates simple harmonic motion, a type of periodic motion where the restoring force is directly proportional to the displacement. The force that pulls or pushes the mass back toward its equilibrium position can be described by Hooke's Law:\[ F = -kx \]Where:
  • \( F \) is the force exerted by the spring.
  • \( k \) is the spring constant (a measure of the spring's stiffness).
  • \( x \) is the displacement from the equilibrium position.
This system oscillates when set in motion, and its behavior can be predicted using certain formulas, especially the frequency formula discussed previously. A critical aspect is that the system's motion is purely dependent on the mass and the spring constant, not on factors such as amplitude, provided the amplitude remains small. Such systems are found everywhere in the world around us, from car suspensions to the function of clocks. Understanding these systems helps in designing various practical applications that rely on controlled oscillations and vibrations.
Physics Problem Solving
Tackling physics problems, like understanding the frequency of a mass-spring system, requires breaking down the problem into manageable parts. Here's a general approach for solving such problems related to oscillations:
  • **Understand the Problem**: Clearly define what is given and what needs to be found. In the original exercise, the frequency of a spring system needed to be calculated with updated mass values.
  • **Recall Relevant Formulas**: Identify which physics formulas apply to the situation. For oscillation problems, the frequency formula \( f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \) is key.
  • **Manipulate the Math**: Rearrange equations as needed to solve for the unknown. In this case, you manipulate the relationship between frequency and mass to find the new frequencies without needing the spring constant explicitly.
  • **Calculate Carefully**: When performing calculations, ensure accuracy, especially when dealing with square roots and ratios.
  • **Analyze Results**: Ensure results make sense logically. Added mass leads to lower frequency, while reduced mass gives higher frequency. Cross-check your calculations by considering this relationship.
This structured approach not only helps solve specific physics problems but also strengthens overall problem-solving skills for diverse scientific inquiries.

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Most popular questions from this chapter

If an object on a horizontal, frictionless surface is attached to a spring, displaced, and then released, it will oscillate. If it is displaced 0.120 m from its equilibrium position and released with zero initial speed, then after 0.800 s its displacement is found to be 0.120 m on the opposite side, and it has passed the equilibrium position once during this interval. Find (a) the amplitude; (b) the period; (c) the frequency.

A large, 34.0-kg bell is hung from a wooden beam so it can swing back and forth with negligible friction. The bell's center of mass is 0.60 m below the pivot. The bell's moment of inertia about an axis at the pivot is 18.0 kg \(\cdot\) m\(^2\). The clapper is a small, 1.8-kg mass attached to one end of a slender rod of length \(L\) and negligible mass. The other end of the rod is attached to the inside of the bell; the rod can swing freely about the same axis as the bell. What should be the length \(L\) of the clapper rod for the bell to ring silently\(-\)that is, for the period of oscillation for the bell to equal that of the clapper?

A 1.35-kg object is attached to a horizontal spring of force constant 2.5 N/cm. The object is started oscillating by pulling it 6.0 cm from its equilibrium position and releasing it so that it is free to oscillate on a frictionless horizontal air track. You observe that after eight cycles its maximum displacement from equilibrium is only 3.5 cm. (a) How much energy has this system lost to damping during these eight cycles? (b) Where did the "lost" energy go? Explain physically how the system could have lost energy.

An 85.0-kg mountain climber plans to swing down, starting from rest, from a ledge using a light rope 6.50 m long. He holds one end of the rope, and the other end is tied higher up on a rock face. Since the ledge is not very far from the rock face, the rope makes a small angle with the vertical. At the lowest point of his swing, he plans to let go and drop a short distance to the ground. (a) How long after he begins his swing will the climber first reach his lowest point? (b) If he missed the first chance to drop off, how long after first beginning his swing will the climber reach his lowest point for the second time?

A 5.00-kg partridge is suspended from a pear tree by an ideal spring of negligible mass. When the partridge is pulled down 0.100 m below its equilibrium position and released, it vibrates with a period of 4.20 s. (a) What is its speed as it passes through the equilibrium position? (b) What is its acceleration when it is 0.050 m above the equilibrium position? (c) When it is moving upward, how much time is required for it to move from a point 0.050 m below its equilibrium position to a point 0.050 m above it? (d) The motion of the partridge is stopped, and then it is removed from the spring. How much does the spring shorten?

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