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Consider a particle of mass m moving in two dimensions,

Chapter 13, Problem 13.10

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QUESTION:

Consider a particle of mass m moving in two dimensions, subject to a force \(\mathbf{F}=-k x \hat{\mathbf{x}}+K \hat{\mathbf{y}}\), where k and K are positive constants. Write down the Hamiltonian and Hamilton's equations, using x and y as generalized coordinates. Solve the latter and describe the motion.

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QUESTION:

Consider a particle of mass m moving in two dimensions, subject to a force \(\mathbf{F}=-k x \hat{\mathbf{x}}+K \hat{\mathbf{y}}\), where k and K are positive constants. Write down the Hamiltonian and Hamilton's equations, using x and y as generalized coordinates. Solve the latter and describe the motion.

ANSWER:

Step 1 of 4

Consider the given data as follows.

The force, \(\overrightarrow F  =  - kx\widehat x + K\widehat y\)

To find the potential \(\left( U \right)\), use the following equation.

\(\overrightarrow F  =  - \nabla U\)

Thus,

\({F_x} =  - \frac{{\partial U}}{{\partial x}}\)

And

\({F_y} =  - \frac{{\partial U}}{{\partial y}}\)

Therefore, the potential is,

\(U =  - \int {{F_x}dx}  - \int {{F_y}dy} \)

\( =  - \left( { - k} \right)\int {xdx}  - K\int {dy} \)

\( = \frac{{k{x^2}}}{2} – Ky\)

Now, kinetic energy can be defined as follows.

\(T = \frac{1}{2}m\left( {{{\dot x}^2} + {{\dot y}^2}} \right)\)

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