Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

(a) Suppose you cut a massless ideal spring in half. If the full spring had a force constant k, what is the force constant of each half, in terms of \(k\)? (\(Hint\): Think of the original spring as two equal halves, each producing the same force as the entire spring. Do you see why the forces must be equal?) (b) If you cut the spring into three equal segments instead, what is the force constant of each one, in terms of \(k\)?

Short Answer

Expert verified
For half-spring, \( k_{half} = 2k \); for one-third spring, \( k_{third} = 3k \).

Step by step solution

01

Understanding Hooke's Law

Hooke's Law states that the force exerted by a spring is proportional to the displacement and the spring constant: \( F = kx \). Here, \( k \) is the spring constant that quantifies the spring's stiffness.
02

Analyzing a Spring Cut in Half

When you cut a spring in half, each half still produces the same overall force when stretched or compressed by a given amount, as the total force is always needed to restore the system to equilibrium. Thus, if the original full-length spring has a spring constant \( k \) and is viewed as two springs in series, the force constant for each half can be determined.
03

Deriving the Force Constant for Half a Spring

For two springs in series, the effective spring constant \( k_{eff} \) is given by \( \frac{1}{k_{eff}} = \frac{1}{k_1} + \frac{1}{k_2} \). Assuming each half has the same spring constant \( k_{half} \), we have \( \frac{1}{k} = \frac{1}{k_{half}} + \frac{1}{k_{half}} = \frac{2}{k_{half}} \). Solving this gives \( k_{half} = 2k \).
04

Spring Cut into Three Equal Segments

When the spring is cut into three equal segments, they must all work together when placed in series to equal the original spring constant \( k \).
05

Deriving the Force Constant for One Third of a Spring

Using the formula for springs in series, \( \frac{1}{k} = \frac{1}{k_1} + \frac{1}{k_2} + \frac{1}{k_3} \). Assuming each of the three segments has the same spring constant \( k_{third} \), we have \( \frac{1}{k} = \frac{3}{k_{third}} \). Solving this results in \( k_{third} = 3k \).

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!

Key Concepts

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

Hooke's Law
Hooke's Law is a fundamental principle in physics that describes the behavior of springs. It states that the force required to compress or extend a spring is directly proportional to the displacement it experiences. This can be mathematically expressed as \( F = kx \), where \( F \) is the force applied to the spring, \( k \) is the spring constant, and \( x \) is the displacement from the spring's equilibrium position. The spring constant, \( k \), is a measure of a spring's stiffness. The larger the value of \( k \), the stiffer the spring and the more force is needed to achieve the same displacement.

Understanding Hooke's Law is crucial when working with springs, as it allows you to calculate the force needed for a specific displacement, which is essential in many engineering and physics applications. It also enables the determination of the spring constant \( k \), which is a characteristic of the spring itself and remains constant unless the spring is physically altered.
Series Springs
When springs are connected in series, their overall behavior changes compared to a single spring. In this configuration, each spring contributes to the total displacement when a force is applied. As a result, the system is less stiff as compared to individual springs alone. The effective spring constant for springs in series can be found using the formula: \[ \frac{1}{k_{eff}} = \frac{1}{k_1} + \frac{1}{k_2} + \ldots + \frac{1}{k_n} \] where \( k_{eff} \) is the effective spring constant of the entire system, and \( k_1, k_2, \ldots, k_n \) are the constants of individual springs.

For example, if you cut a spring into two equal halves and place them in series, the system as a whole behaves like a spring with a smaller spring constant than the original. When a spring is split into multiple segments and placed in series, each segment contributes equally to reduce the overall stiffness of the spring system. This principle was used in the exercise to determine that if a spring is cut into halves or thirds, each resulting piece has a different spring constant than any single piece would exhibit alone.
Spring Stiffness
Spring stiffness is an essential characteristic of a spring, denoted by the spring constant \( k \). This stiffness determines how much force is needed to stretch or compress a spring by a given distance. Spring stiffness directly affects how the spring behaves in various configurations, such as when springs are arranged in series or parallel.

In the exercise, when the spring is cut into different segments, the stiffness of each new spring segment changes in relation to the original spring. For instance, if the spring is cut into two halves and treated as series springs, each half has a spring constant of \( 2k \), meaning each part is independently stiffer and compensates for being in series by providing half the force. However, cutting the spring into three pieces results in each having a spring constant of \( 3k \) when put in series, showing that smaller segments proportionally increase the stiffness to maintain the spring's behavior.
  • This illustrates how manipulating spring configuration can dramatically change system attributes.
  • Understanding spring stiffness is integral to designing mechanical systems involving springs.
Overall, these factors highlight how spring stiffness and series configurations interplay to impact the mechanical behavior of springs.

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

One end of a horizontal spring with force constant 130.0 N/m is attached to a vertical wall. A 4.00-kg block sitting on the floor is placed against the spring. The coefficient of kinetic friction between the block and the floor is \(\mu_k = 0.400\). You apply a constant force \(\overrightarrow{F}\) to the block. \(\overrightarrow{F}\) has magnitude \(F = 82.0\) N and is directed toward the wall. At the instant that the spring is compressed 80.0 cm, what are (a) the speed of the block, and (b) the magnitude and direction of the block's acceleration?

You are asked to design spring bumpers for the walls of a parking garage. A freely rolling 1200-kg car moving at 0.65 m/s is to compress the spring no more than 0.090 m before stopping. What should be the force constant of the spring? Assume that the spring has negligible mass.

When its 75-kW (100-hp) engine is generating full power, a small single-engine airplane with mass 700 kg gains altitude at a rate of 2.5 m/s (150 m/min, or 500 ft/min). What fraction of the engine power is being used to make the airplane climb? (The remainder is used to overcome the effects of air resistance and of inefficiencies in the propeller and engine.)

Based on the given data, how does the energy used in biking 1 km compare with that used in walking 1 km? Biking takes (a) \\(\frac{1}{3}\\) of the energy of walking the same distance; (b) the same energy as walking the same distance; (c) 3 times the energy of walking the same distance; (d) 9 times the energy of walking the same distance.

You are a member of an Alpine Rescue Team. You must project a box of supplies up an incline of constant slope angle \(\alpha\) so that it reaches a stranded skier who is a vertical distance \(h\) above the bottom of the incline. The incline is slippery, but there is some friction present, with kinetic friction coefficient \(\mu_k\). Use the work\(-\) energy theorem to calculate the minimum speed you must give the box at the bottom of the incline so that it will reach the skier. Express your answer in terms of \(g\), \(h\), \(\mu_k\), and \(\alpha\).

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