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The motion of a particle is given by $$ y=4 \sin \omega t+8 \sin \left(\omega t+\frac{\pi}{3}\right) $$ The motion of particle is: (a) S.H.M. (b) not S.H.M. (c) periodic but not S.H.M. (d) none of the above

Short Answer

Expert verified
(a) S.H.M.

Step by step solution

01

Identify S.H.M.

Simple Harmonic Motion (S.H.M.) is defined by a sinusoidal motion that can be expressed in the form \( y = A \sin(\omega t + \phi) \) or \( y = A \cos(\omega t + \phi) \). This indicates a single sine or cosine function.
02

Combine the Equation Terms

We need to simplify the given expression: \[ y = 4 \sin \omega t + 8 \sin \left(\omega t + \frac{\pi}{3}\right)\]We can use the trigonometric identity for sine addition to combine these terms.
03

Use Trigonometric Identities

The trigonometric identity for the sine of a sum is:\[ \sin(a+b) = \sin a \cos b + \cos a \sin b \]Applying this identity to \( 8 \sin \left(\omega t + \frac{\pi}{3}\right) \):\[8 \sin \omega t \cos \frac{\pi}{3} + 8 \cos \omega t \sin \frac{\pi}{3}\]Simplifying this, because \( \cos \frac{\pi}{3} = \frac{1}{2} \) and \( \sin \frac{\pi}{3} = \frac{\sqrt{3}}{2} \), gives: \[4 \sin \omega t + 8 \cdot \frac{1}{2} \sin \omega t + 8 \cdot \frac{\sqrt{3}}{2} \cos \omega t\]Thus, \[8 \sin \omega t + 4\sqrt{3} \cos \omega t\].
04

Analyze Resulting Equation

The combined expression:\[8 \sin \omega t + 4\sqrt{3} \cos \omega t\]can be seen as a result of adding two sinusoidal components with different phases. This can be rewritten as a single sine function using the form \( R \sin(\omega t + \phi) \).
05

Determine Type of Motion

The motion can be considered simple harmonic if we can express it as a single sine or cosine function. Since the transformed expression is a combination that fits this form, the motion is S.H.M.

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Key Concepts

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

Trigonometric Identities
Trigonometric identities are mathematical shortcuts that help simplify complex trigonometric expressions. These are essential in various calculations invovling angles and periodic functions. One key identity used in this context is the sine addition formula, which allows us to break down or combine trigonometric functions involving sums of angles.

For example, the formula for the sine of a sum:
  • \( \sin(a + b) = \sin a \cos b + \cos a \sin b \)
This identity helps to combine multiple sine terms into a single expression, which can simplify understanding the motion of a particle.
In the original exercise, we applied this by breaking down the term \( 8 \sin\left(\omega t + \frac{\pi}{3}\right) \). This application highlights how trigonometric identities can transform complex combinations into manageable forms, making it easier to identify the nature of the motion.
Sinusoidal Motion
Sinusoidal motion refers to motion that follows a pattern described using sine or cosine functions. This type of motion is common in real-world phenomena like waves, vibrations, and oscillatory systems.

Each sinusoidal motion can be described by a unique equation of the form:
  • \( y = A \sin(\omega t + \phi) \)
  • \( y = A \cos(\omega t + \phi) \)
Where:
  • \( A \) is the amplitude.
  • \( \omega \) is the angular frequency.
  • \( \phi \) is the phase angle, indicating how the wave has shifted horizontally.
When a particle's motion fits these equations, such as in Simple Harmonic Motion (S.H.M.), its movement is perfectly sinusoidal.
In the given problem, after simplifying through trigonometric identities, we see the final expression as a composite of sinusoidal components, leading to its classification as S.H.M. despite its complex appearance.
Superposition of Waves
The superposition of waves is a principle that describes how waves overlapping in space add up to form a new wave pattern. This is crucial in understanding complex wave behaviors in physics and engineering.

Simply put, when two or more waves meet, their amplitudes are combined to result in a new waveform. Depending on their phase relationships, this can lead to constructive or destructive interference.
In the context of the problem, the equation \( y = 4 \sin \omega t + 8 \sin \left(\omega t + \frac{\pi}{3}\right) \) represents two waveforms superposing. The use of trigonometric identities simplifies this superposition, effectively reducing it to a single sinusoidal expression.
This amalgamation allows us to understand that even though the original motion was a combination of different phases, the overall behavior still adheres to the nature of Simple Harmonic Motion. This emphasizes how different waves can blend into coherent waveforms, illustrating the power of superposition in wave motion.

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