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Statement-1: If force acting on a particle is given by \(F=-k x^{2}\), then the motion of the particle is periodic but not the simple harmonic oscillation. Statement-2 : For the simple harmonic oscillation the force must be proportional to the displacement of the particle from the mean position.

Short Answer

Expert verified
Statement-1 is true; Statement-2 is true and correctly explains Statement-1.

Step by step solution

01

Understanding Statement-1

Statement-1 claims that a force described by \(F = - k x^2\) leads to periodic motion, but the motion is not simple harmonic. Let's break it down: periodic motion means the particle moves in a repeated pattern over time, while simple harmonic motion (SHM) requires that the force be directly proportional to the displacement (\(F = -kx\)). Since the given force depends on \(x^2\) instead of \(x\), it's not SHM.
02

Understanding Statement-2

Statement-2 says for motion to be simple harmonic, the force must be proportional to the displacement (i.e., \(F = -kx\)). This is true; in SHM, the restoring force depends linearly on the displacement from equilibrium. This statement provides the standard definition for simple harmonic motion.
03

Verifying the Relationship Between Force and SHM

Since the force in Statement-1 is \(F = - k x^2\), it is not proportional to \(x\), but to \(x^2\). For the motion to be simple harmonic, the force should be linear in \(x\). Therefore, the motion described in Statement-1 cannot be SHM according to the definition given in Statement-2.
04

Determining the Correctness of Statements

We confirm that Statement-1 correctly describes a type of periodic motion that isn't simple harmonic, and Statement-2 correctly states the condition for SHM. Thus, Statement-2 correctly explains why the motion in Statement-1 is not simply harmonic.

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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 where the restoring force acting on an object is directly proportional to the displacement from its equilibrium position. This relationship is mathematically written as \( F = -kx \), where \( F \) is the force, \( k \) is a constant known as the force constant, and \( x \) is the displacement. This specific formula shows that the force is a linear function of \( x \). The negative sign indicates that the force acts in the opposite direction of the displacement, pulling the object back to its equilibrium position.
The structure of this force gives rise to some important characteristics of SHM:
  • The motion is symmetric about the equilibrium point.
  • The period of motion (the time it takes to complete one full cycle) remains constant.
  • The motion is sinusoidal, often described using sine or cosine functions.
SHM can be observed in systems like vibrating springs, pendulums, and even in certain electronic circuits. It's important to distinguish it from other periodic motions by checking if the force-displacement relationship meets the criteria mentioned above.
Restoring Force
The concept of restoring force is central to understanding many types of periodic motions, including simple harmonic motion. A restoring force is any force that tends to restore a system to its equilibrium position when it is displaced. In the context of SHM, this force is proportional and opposite to the displacement, as represented by \( F = -kx \).
This means the further you pull or push the object from its equilibrium position, the stronger the force trying to bring it back.
  • Proportionate: In SHM, the force increases linearly with distance, meaning a small displacement results in a small force, and a large displacement results in a large force.
  • Opposing: The negative sign in \( F = -kx \) indicates opposition, always acting to bring the object back to center.
Such a force ensures that when the particle overshoots the equilibrium, it experiences a force pushing it back, leading to oscillations back and forth about the equilibrium position. This repetitive cycle creates the periodic nature of the motion.
Displacement
Displacement in the context of periodic motion and SHM specifically refers to the distance a particle is from its equilibrium position at any given point in time. It's a vector quantity, meaning it has both magnitude and direction.
In simple harmonic motion, displacement is crucial as it directly influences the magnitude of the restoring force (\( F = -kx \)).
  • Maximum Displacement: Known as the amplitude of motion. It represents the furthest point the object reaches from the equilibrium position.
  • Zero Displacement: When the object is at its mean or equilibrium position, resulting in zero net force acting on the object.
  • Sign of Displacement: Positive or negative displacement indicates direction - whether the object is on one side or the other of the equilibrium.
Visualizing displacement can be facilitated by imagining a spring being compressed and extended around an equilibrium position. At any moment, the distance from this resting point is the displacement, dictating how strong the force is and which direction it pushes or pulls.

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Most popular questions from this chapter

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