Question:

The Hamiltonian for a one-dimensional system with mass m m , position q q , and momentum p p is: H(p,q)=p22m+q2A(q) H(p, q) = \frac{p^2}{2m} + q^2 A(q) where A(q) A(q) is a real function of q q . If md2qdt2=5qA(q), m \frac{d^2 q}{dt^2} = -5q A(q), then dA(q)dq=nA(q)q. \frac{d A(q)}{d q} = n \frac{A(q)}{q}. The value of n n (in integer) is:

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For a system described by a Hamiltonian with a position-dependent potential, the equation of motion and the Hamiltonian's partial derivatives can be used to find relationships between the function A(q) A(q) and its derivative.
Updated On: Apr 8, 2025
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Solution and Explanation

1. Using the Hamiltonian:
The Hamiltonian of the system is given by:

H(p,q)=p22m+q2A(q) H(p, q) = \frac{p^2}{2m} + q^2 A(q)

The Hamiltonian represents the total energy of the system, which is a sum of kinetic and potential energies.

2. Equations of motion:
The equations of motion are given by Hamilton's equations. For position q q and momentum p p , we have:

dqdt=Hp=pm \frac{dq}{dt} = \frac{\partial H}{\partial p} = \frac{p}{m}

and

dpdt=Hq=2qA(q)q2dA(q)dq \frac{dp}{dt} = -\frac{\partial H}{\partial q} = -2q A(q) - q^2 \frac{dA(q)}{dq}

3. Substitute the equation of motion:
According to the problem, we are given that:

md2qdt2=5qA(q) m \frac{d^2 q}{dt^2} = -5q A(q)

Using dqdt=pm \frac{dq}{dt} = \frac{p}{m} , we get:

md2qdt2=ddt(pm)=dpdt m \frac{d^2 q}{dt^2} = \frac{d}{dt} \left( \frac{p}{m} \right) = \frac{dp}{dt}

Substituting the expression for dpdt \frac{dp}{dt} :

md2qdt2=2qA(q)q2dA(q)dq m \frac{d^2 q}{dt^2} = -2q A(q) - q^2 \frac{dA(q)}{dq}

Comparing this with the given equation:

2qA(q)q2dA(q)dq=5qA(q) -2q A(q) - q^2 \frac{dA(q)}{dq} = -5q A(q)

4. Solve for dA(q)dq \frac{dA(q)}{dq} :
Simplifying:

q2dA(q)dq=3qA(q)dA(q)dq=3A(q)q -q^2 \frac{dA(q)}{dq} = -3q A(q) \quad \Rightarrow \quad \frac{dA(q)}{dq} = \frac{3A(q)}{q}

Comparing with dA(q)dq=nA(q)q \frac{dA(q)}{dq} = n \frac{A(q)}{q} , we find:

n=3 n = \boxed{3}

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