← 2019 Paper 2

UPSC 2019 Maths Optional Paper 2 Q7a — Step-by-Step Solution

15 marks · Section B

Hamilton's equations · Mechanics & Fluid Dynamics · asked 10× in 13 yrs · Read the full method →

Question

Using Hamilton’s equation, find the acceleration for a sphere rolling down a rough inclined plane, if xx be the distance of the point of contact of the sphere from a fixed point on the plane.

Technique

Build L\mathcal L with the rolling constraint folded in (ϕ˙=x˙/r\dot\phi=\dot x/r), pass to H=T+VH=T+V in terms of (x,p)(x,p), then apply Hamilton’s equations x˙=pH\dot x=\partial_p H, p˙=xH\dot p=-\partial_x H and combine.

Solution

Setup. Uniform solid sphere, mass MM, radius rr, moment of inertia I=25Mr2I=\tfrac25 Mr^2, rolling without slipping down a plane inclined at angle θ\theta to the horizontal. Let xx be the distance of the contact point along the plane from a fixed point (down-plane positive). Rolling: the spin ϕ\phi satisfies x=rϕx=r\phi, so ϕ˙=x˙/r\dot\phi=\dot x/r. There is a single generalised coordinate xx.

Step 1 — Lagrangian (to build the Hamiltonian)

Kinetic energy (translation + rotation, with ϕ˙=x˙/r\dot\phi=\dot x/r):

T=12Mx˙2+12Iϕ˙2=12Mx˙2+12(25Mr2)x˙2r2=12Mx˙2(1+25)=710Mx˙2.T=\tfrac12 M\dot x^2+\tfrac12 I\dot\phi^2=\tfrac12 M\dot x^2+\tfrac12\Big(\tfrac25 Mr^2\Big)\frac{\dot x^2}{r^2}=\tfrac12 M\dot x^2\Big(1+\tfrac25\Big)=\tfrac{7}{10}M\dot x^2.

Potential energy (height drops by xsinθx\sin\theta):

V=Mgxsinθ.V=-Mgx\sin\theta.

So L=TV=710Mx˙2+Mgxsinθ.\mathcal L=T-V=\tfrac{7}{10}M\dot x^2+Mgx\sin\theta.

Step 2 — Generalised momentum and Hamiltonian

p=Lx˙=75Mx˙  x˙=5p7M.p=\frac{\partial\mathcal L}{\partial\dot x}=\frac{7}{5}M\dot x\ \Longrightarrow\ \dot x=\frac{5p}{7M}.

The Hamiltonian H=px˙LH=p\dot x-\mathcal L (a natural system, so H=T+VH=T+V expressed in pp):

H=p2275MMgxsinθ=5p214MMgxsinθ.H=\frac{p^2}{2\cdot\frac{7}{5}M}-Mgx\sin\theta=\frac{5p^2}{14M}-Mgx\sin\theta.

Step 3 — Hamilton’s equations

x˙=Hp=5p7M,\dot x=\frac{\partial H}{\partial p}=\frac{5p}{7M}, p˙=Hx=Mgsinθ.\dot p=-\frac{\partial H}{\partial x}=Mg\sin\theta.

Step 4 — Acceleration

From x˙=5p7M\dot x=\dfrac{5p}{7M}, differentiate: x¨=5p˙7M=57M(Mgsinθ)\ddot x=\dfrac{5\dot p}{7M}=\dfrac{5}{7M}\,(Mg\sin\theta).

Answer

  x¨=57gsinθ.  \boxed{\;\ddot x=\frac{5}{7}\,g\sin\theta.\;}
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