Piano man
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I'm having a bit of difficulty understanding part of this problem:
Using the Hamilton-Jacobi equation find the trajectory and the motion of a particle in the
potential U(r)=-Fx
The Hamilton-Jacobi Equation: \frac{\partial S}{\partial t}+H(q_1,...,q_s;\frac{\partial S}{\partial q_1},...,\frac{\partial S}{\partial q_s};t)=0
Starting off with the Hamiltonian:
<br /> H(p_x,p_y,p_z,x,y,z)=\frac{p_x^2}{2m}-Fx+\frac{p_y^2}{2m}+\frac{p_z^2}{2m}
From HJE, since y and z are cyclic,
<br /> S(x,y,z;p_x,p_y,p_z;t)=-Et+p_yy+p_zz+S(x,p_x)
All this is grand, but the next step in the solutions I have say that we can now say that <br /> E=p_x+\frac{p_y^2}{2m}+\frac{p_z^2}{2m}
I don't see where this comes from.
Any ideas?
Thanks
Using the Hamilton-Jacobi equation find the trajectory and the motion of a particle in the
potential U(r)=-Fx
The Hamilton-Jacobi Equation: \frac{\partial S}{\partial t}+H(q_1,...,q_s;\frac{\partial S}{\partial q_1},...,\frac{\partial S}{\partial q_s};t)=0
Starting off with the Hamiltonian:
<br /> H(p_x,p_y,p_z,x,y,z)=\frac{p_x^2}{2m}-Fx+\frac{p_y^2}{2m}+\frac{p_z^2}{2m}
From HJE, since y and z are cyclic,
<br /> S(x,y,z;p_x,p_y,p_z;t)=-Et+p_yy+p_zz+S(x,p_x)
All this is grand, but the next step in the solutions I have say that we can now say that <br /> E=p_x+\frac{p_y^2}{2m}+\frac{p_z^2}{2m}
I don't see where this comes from.
Any ideas?
Thanks