Let a particle of unit mass be subject to a force x- x3 where x is its displacement from the coordinate origin. (a) Find the equilibrium points, and tell whether they are stable or unstable. (b) Calculate the totalenergy of the particle, and show that it is a conserved quantity. (C) Calculate the trajectories of the particle in phase space.
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- Set up the integrals to find the ycoordinate of the center of mass for a region of density (x;y)inside the circle x^2 + y^2 = 4 and below y = sqrt (2)Which of the following is the conserved quantity if the system having Lagrangian L= = m(x² + y²) – ² k(x² + y²). (a) Px (b) Py (c) L₂ (d) NoneAs shown in the figure below,a small ball of mass m is attached to the free end of an ideal string of length 7 that is hanging from the ceiling at point S. The ball is moved away from the vertical and released. At the instant shown in the figure, the ball is at an angle ✪ (t) with respect to the vertical. Suppose the angle is small throughout the motion. zero of potential g pivot S 1 mVerify that each of the following force fields is conservative. Then find, for each, a scalar potential o such that F = -Vo. F = (3x²yz − 3y)i + (x³z − 3x)j + (x³y + 2z)k.prove this force are conserved F(x,y)=2a(x-y)i-a(2x-y)j Where a is constant(a) For one-dimensional motion of a particle of mass m acted upon by a force F(x), obtain the formal solution to the trajectory x(t) in the inverse form: m = ₂√ 2 {E – V(x)} where V (x) is the potential energy and x0 is the position at t = 0. (b) If the force, F(x) is a constant then what is the equation of the particles trajectory (x vs t). t(x): = dxConsider a thin disc of radius R and consisting of a material with constant mass density (per unit of area) g. Use cylindrical coordinates, with the z-axis perpendicular to the plane of the disc, and the origin at the disc's centre. We are going to calculate the gravitational potential, and the gravitational field, in points on the z-axis only. 1. Show that the gravitational potential 4(2) set up by that disc is given by p(2) = 2mGg | dr'; make sure to explain where the factor 27 comes from, and where the factor r' in the integrand comes from. 2. Evaluate this integral. 3. Approximate p(z), both for 0 R (i.e., for points very far away). You will need the following Taylor approximation: VI+x=1++O(x²), applied in different ways... .A frictionless spring with a 5-kg mass can be held stretched 1.2 meters beyond its natural length by a force of 90 newtons. If the mass begins at its equilibrium position, but an upward push gives it ar initial velocity of 2.5 m/sec, find the position of the mass after t seconds (where the upward direction is presumed to be positive). Express your solution as a real-valued function. Use g 9.8-m, as needed. sec metersTwo particles, each of mass m, are connected by a light inflexible string of length l. The string passes through a small smooth hole in the centre of a smooth horizontal table, so that one particle is below the table and the other can move on the surface of the table. Take the origin of the (plane) polar coordinates to be the hole, and describe the height of the lower particle by the coordinate z, measured downwards from the table surface. Here, the total force acting on the mass which is on the table is -T r^ (r hat). Why?The Newton–Raphson method for finding the stationary point(s) Rsp of a potential energy surface V is based on a Taylor-series expansion around a guess, R0. Similarly, the velocity Verlet algorithm for integrating molecular dynamics trajectories [xt, vt] is based on a Taylor-series expansion around the initial conditions, [x0, v0]. Both of these methods rely strictly on local information about the system. How many derivatives do we need to compute in order to apply them?Consider the nonconservative mass-spring system governed by ï +2 +26x = 0, x(0) = 1, ż(0) = 4 (a) Find the solution z(t) and its derivative i(t), and evaluate x(7/5) and (7/5). (b) Calculate the total energy E (t) of the system when t = π/5. (c) Calculate the energy loss in the system due to friction in the time interval from t = 0 to t = π/5. no.Consider a particle of mass m moving in 1-dimension under a piecewise-constant po- tential. In region I, that corresponds to x 0. In region II, that corresponds to x > 0 the potential energy is V1(x) = 0. The particle is shot from = -∞ in the positive direction with energy E > Vo > 0. See the figure in the next page for a representation of V(x) as a function of x. Also shown in the graph (green dashed line) the energy E of the particle. (a) Which of the following functions corresponds to the wavefunction 1(x) in region I? (a1) Aeikiæ + Be-iki¤ ; (а2) Ае\1 + Bе-кӕ (a3) Aeikræ (а4) Ве- кта (b) Which of the following functions corresponds to the wavefunction 1(x) in region II? (b1) Сеkп* + De-ikr (62) C'e*I1* + De-*1¤