3. Consider a single particle of mass m in spherical coordinates, with the kinetic energy lees so that the vertical separation between them is constant. Some possibly useful formulas: F = ma, FkHkFN, F = P₁ T = p = mv, r2 sin² 0 (a) Write the hamiltonian H and find Hamilton's equations in the case of a central potential V(r). Discuss how the z axis of spherical coordinates should be chosen to simplify the problem to a 2D situation. Write the corresponding 2D hamiltonian. Recover the standard expression for dt in terms of dr, r, E, V(r), l, m. 1 2m (b) Consider now V(r) = V₁(r)â f, where â is a fixed unit vector and is the unit vector along the direction of F. V₁ (r) <0 is a function of the distance r = r. (i) Choose an appropriate direction for the z axis, write the hamiltonian H, and find Hamilton's equations. Show that one component of angular momentum is conserved. (ii) Propose a circular motion solution for the equations of motion, with its axis of rotation along â. Find a condition of the form fr(ro) = fe(80) P + relating the constant values r = ro and 0 = 0o. Find explicit expressions for po and w in terms of ro, 0o, m, V₁ (ro) where w is the angular speed of the motion. (iii) Consider V₁ (r) = -Ae-/, with A, λ> 0 constants, show that in this case o can be chosen arbitrarily, and compute ro, Po, w in terms of 0o, m, A, A. (iv) Consider V₁ (r) = -Bra, with B, a>0 constants, show that in this case ro can be chosen arbitrarily, that 00 is independent of ro, and compute fo, Po, in terms of ro, m, B, a. 0≤Fs ≤s FN デューデ F21 = - Gm₁m2 -2. Q Search 21 F21 = Q1Q21-3, L = F xp, Ñ = ŕ x F = 1 (0)

3. Consider a single particle of mass m in spherical coordinates, with the kinetic energy lees so that the vertical separation between them is constant. Some possibly useful formulas: F = ma, FkHkFN, F = P₁ T = p = mv, r2 sin² 0 (a) Write the hamiltonian H and find Hamilton's equations in the case of a central potential V(r). Discuss how the z axis of spherical coordinates should be chosen to simplify the problem to a 2D situation. Write the corresponding 2D hamiltonian. Recover the standard expression for dt in terms of dr, r, E, V(r), l, m. 1 2m (b) Consider now V(r) = V₁(r)â f, where â is a fixed unit vector and is the unit vector along the direction of F. V₁ (r) <0 is a function of the distance r = r. (i) Choose an appropriate direction for the z axis, write the hamiltonian H, and find Hamilton's equations. Show that one component of angular momentum is conserved. (ii) Propose a circular motion solution for the equations of motion, with its axis of rotation along â. Find a condition of the form fr(ro) = fe(80) P + relating the constant values r = ro and 0 = 0o. Find explicit expressions for po and w in terms of ro, 0o, m, V₁ (ro) where w is the angular speed of the motion. (iii) Consider V₁ (r) = -Ae-/, with A, λ> 0 constants, show that in this case o can be chosen arbitrarily, and compute ro, Po, w in terms of 0o, m, A, A. (iv) Consider V₁ (r) = -Bra, with B, a>0 constants, show that in this case ro can be chosen arbitrarily, that 00 is independent of ro, and compute fo, Po, in terms of ro, m, B, a. 0≤Fs ≤s FN デューデ F21 = - Gm₁m2 -2. Q Search 21 F21 = Q1Q21-3, L = F xp, Ñ = ŕ x F = 1 (0)