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Problem A: Energy conservation Mechanical systems are determined by the energy function H(x,y), a function of two variables. Here, x is the position and y is the momentum. The equations of motion for the curve r(t) = (x(t),y(t)) are
x'(t) = Hy(x,y)
y'(t) = -Hx(x,y)
which are called Hamilton equations. These equations tell what the
velocity vector r'(t) = (x'(t),y'(t)) is at a given point. a) (4 points) Using the chain rule, verify that in full generality, the energy of a Hamiltonian system is preserved: for every path r(t) = (x(t),y(t)) solving the system, we have H(x(t),y(t)) = constb) (2 points) What is the relation between the level curves of the function H(x,y) and the solution curves r(t) = (x(t),y(t)) of the system? c) (2 points) Determine whether the Hamiltonian system with energy H(x,y) = x4 + y4 can have paths which go to infinity. d) (2 points) Determine whether the Hamiltonian system with energy H(x,y) = x4 - y4 has solution paths for which the position goes to infinity. Here are two examples of mechanical systems. |
| The harmonic oscillator | The pendulum |
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H(x,y) = x2/2 + y2/2The Hamilton equations are
dx/dt = y
dy/dt = - x
It has the solution x(t) = sin(t),y(t) = cos(t).
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H(x,y) = -cos(x) + y2/2The Hamilton equations are
dx/dt = y
dy/dt = -sin(x)
Its solution can not be described by elementary
functions.
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