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Question: A particle of mass m oscillates along x-axis according to equation x = asinωt. The nature of the gra...

A particle of mass m oscillates along x-axis according to equation x = asinωt. The nature of the graph between momentum and displacement of the particle is

A

A straight line

B

A circle

C

An ellipse

D

A parabola

Answer

An ellipse

Explanation

Solution

The displacement of the particle is given by x=asin(ωt)x = a \sin(\omega t). The velocity is the time derivative of displacement: v=dxdt=aωcos(ωt)v = \frac{dx}{dt} = a \omega \cos(\omega t). Momentum is given by p=mvp = mv, so p=m(aωcos(ωt))=maωcos(ωt)p = m(a \omega \cos(\omega t)) = ma \omega \cos(\omega t). From the displacement equation, we can express sin(ωt)\sin(\omega t) as xa\frac{x}{a}. From the momentum equation, we can express cos(ωt)\cos(\omega t) as pmaω\frac{p}{ma \omega}. Using the fundamental trigonometric identity sin2(θ)+cos2(θ)=1\sin^2(\theta) + \cos^2(\theta) = 1, we substitute θ=ωt\theta = \omega t: sin2(ωt)+cos2(ωt)=1\sin^2(\omega t) + \cos^2(\omega t) = 1 Substituting the expressions for sin(ωt)\sin(\omega t) and cos(ωt)\cos(\omega t): (xa)2+(pmaω)2=1\left(\frac{x}{a}\right)^2 + \left(\frac{p}{ma \omega}\right)^2 = 1 This equation can be rewritten as: x2a2+p2(maω)2=1\frac{x^2}{a^2} + \frac{p^2}{(ma \omega)^2} = 1 This is the standard form of the equation of an ellipse centered at the origin (0,0)(0,0) in the xpx-p plane. The semi-major/minor axes are aa along the x-axis and maωma\omega along the p-axis.