Animated Solution for Physics - Oscillations: Two simple harmonic motions are represented by the equations
y1=10sin(3πt+4π) and y2=5(sin3πt+3cos3πt).
Their amplitudes are in the ratio of \_\_\_\_\_\_.
Visualized Solution
Analyze the First SHM Equation
The first simple harmonic motion is given by:
y1=10sin(3πt+4π)
Comparing this with the standard equation of SHM: y=Asin(ωt+ϕ)
We can directly read the amplitude of the first motion:
A1=10
Analyze the Second SHM Equation
The second motion is represented by:
y2=5(sin3πt+3cos3πt)
This is a combination of a sine and a cosine function.
To find its amplitude, we need to combine these two perpendicular components.
The Phasor Addition Method
Any expression of the form y=asinωt+bcosωt can be represented as the sum of two perpendicular vectors (phasors):
1. A horizontal vector of magnitude a along the sine axis.
2. A vertical vector of magnitude b along the cosine axis (since cosine leads sine by 2π).
Identify the Component Amplitudes
Expanding the expression for y2:
y2=5sin3πt+53cos3πt
Here, the sine component amplitude is:
a=5
The cosine component amplitude is:
b=53
Calculate the Resultant Amplitude A2
The resultant amplitude A2 is given by the vector sum formula:
A2=a2+b2
Substituting the values:
A2=(5)2+(53)2
Simplify the Square Root
Evaluating the squares:
52=25
(53)2=25×3=75
Adding the terms:
A2=25+75=100
A2=10
Determine the Phase Angle ϕ
The phase angle ϕ of the resultant wave is:
tanϕ=ab=553=3
ϕ=tan−1(3)=60∘=3π rad
Thus, y2=10sin(3πt+3π)
Find the Ratio A2A1
We have:
A1=10
A2=10
The ratio of their amplitudes is:
A2A1=1010=1
Therefore, the ratio is 1:1.
Alternative Trigonometric Method
We can also solve this using the trigonometric identity:
Asinθ+Bcosθ=A2+B2sin(θ+ϕ)
where tanϕ=AB.
This identity is extremely useful for combining harmonic waves in wave optics and AC circuits.
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The Sigma Insight: Simple Harmonic Motion (SHM)
Solution Diagram
Introduction to Superposition of Simple Harmonic Motions
Simple Harmonic Motion (SHM) is one of the most fundamental concepts in physics, describing everything from the swing of a pendulum to the vibration of atoms in a crystal lattice.
Often, a physical system is subjected to multiple harmonic influences simultaneously.
When this happens, we use the Principle of Superposition, which states that the net displacement is the algebraic sum of the individual displacements.
In this problem, we are given two simple harmonic motions represented by the equations:
y1=10sin(3πt+4π)
y2=5(sin3πt+3cos3πt)
Our goal is to find the ratio of their amplitudes, A1:A2.
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Analyzing the First SHM
The first equation is already presented in the standard form of a simple harmonic wave:
y=Asin(ωt+ϕ)
By direct comparison with y1=10sin(3πt+4π), we can immediately identify the key parameters of the first motion:
- Amplitude (A1):10 units
- Angular Frequency (ω1):3π rad/s
- Initial Phase (ϕ1):4π rad
Thus, we have our first amplitude:
A1=10
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Deconstructing the Second SHM
The second equation, y2=5(sin3πt+3cos3πt), is a linear combination of a sine and a cosine function of the same frequency.
To find its net amplitude, we must combine these two terms into a single sinusoidal expression.
Let's first expand the expression:
y2=5sin3πt+53cos3πt
This is of the form:
y=asinωt+bcosωt
where a=5 and b=53.
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The Phasor Addition Method
An elegant way to combine sine and cosine functions of the same frequency is by using phasors (vector representation of harmonic quantities).
Since a cosine wave leads a sine wave by a phase difference of 2π radians (90∘), we can represent them as two perpendicular vectors:
1. A horizontal vector of magnitude a=5 representing the sine component.
2. A vertical vector of magnitude b=53 representing the cosine component.
The resultant vector represents the combined wave, and its length is the resultant amplitude A2.
Using the Pythagorean theorem for perpendicular vectors:
A2=a2+b2
Substituting our values:
A2=(5)2+(53)2
A2=25+25×3
A2=25+75=100
A2=10
Thus, the amplitude of the second SHM is also 10 units.
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Finding the Phase of the Second SHM
To write the complete equation for y2, we can also find the resultant phase angle ϕ: