The displacement of an oscillating particle is given by x = asinωt + bcosωt where a, b and ω are constants. Prove that the particle performs a linear S.H.M. with amplitude A = √a² + b²
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Answers
The displacement of an oscillating particle is given by x = a sin ω t + b cos ω t where a, b and ω are constants.
Prove that the particle performs a linear S.H.M. with amplitude A =
Displacement an oscillating particle is given by x = a sin ω t + b cos ω t where a, b and ω are constants.
Prove that the particle performs a linear S.H.M. with amplitude A =
The position of the particle is given as
y = A = cos ω t + B sin ω t ____( 1)
The Velocity of the particle is given by,
V = = (A cos ω t + B sin ω t)
= - Aω sin ωt + Bω cos ωt
Acceleration of the particle is given by,
A = (- Aω sin ωt + Bω² cos ωt)
= - Aω² cos ωt + Bω² cos ωt
= ω² (A cos ωt + B sin ωt)
= ω² = y
As the acceleration of the particle is directly proportional to the displacement & directed towards mean position... We can understand that tyhe motion is a simple harmonic motion.
Now,
Let amplitude A = r sin ᵠ ___(2)
B = r cos ᵠ ___(3)
By substituting A & B in equation (1), we get↷:
y = r sin ᵠ cos ωt + r cos ᵠ sin ωt
= r (cos ωt sin ᵠ + sin ωt cos ᵠ)
= r sin (ωt + ᵠ)
Squaring (2) & (3) and adding, we have,
A² + B² = r²
= r
Dividing (2) & (3) we have,
= tan ∅
= r
Amplitude = r
QUESTION:-)
The displacement of an oscillating particle is given by x = asinωt + bcosωt where a, b and ω are constants. Prove that the particle performs a linear S.H.M. with amplitude A = √a² + b²?
ANSWER:-)
The displacement of an oscillating particle is given by x = a sin ω t + b cos ω t where a, b and ω are constants.
Prove that the particle performs a linear S.H.M. with amplitude A = a²+b²
Given↷
Displacement an oscillating particle is given by x = a sin ω t + b cos ω t where a, b and ω are constants.
To prove√
Prove that the particle performs a linear S.H.M. with amplitude A = a²+b²
Explanation√
The position of the particle is given as
y = A = cos ω t + B sin ω t ____( 1)
The Velocity of the particle is given by,
V = dt=dy
(A cos ω t + B sin ω t)
= - Aω sin ωt + Bω cos ωt
Acceleration of the particle is given by,
(- Aω sin ωt + Bω² cos ωt)
= - Aω² cos ωt + Bω² cos ωt
= ω² (A cos ωt + B sin ωt)
= ω² = y
As the acceleration of the particle is directly proportional to the displacement & directed towards mean position... We can understand that tyhe motion is a simple harmonic motion.
Now,
Let amplitude A = r sin ᵠ ___(2)
B = r cos ᵠ ___(3)
By substituting A & B in equation (1), we get↷:
y = r sin ᵠ cos ωt + r cos ᵠ sin ωt
= r (cos ωt sin ᵠ + sin ωt cos ᵠ)
= r sin (ωt + ᵠ)
Squaring (2) & (3) and adding, we have,
A² + B² = r²
= r \bf{\sqrt{A² + B²}}
A²+B²
Dividing (2) & (3) we have,
= tan ∅
= r \bf{\sqrt{A² + B²}}
A²+B²
Answer√
Amplitude = r \bf{\sqrt{A² + B²}}
A²+B²