A particle constrained to move along the X-axis in a potential V = kx2, is subjected to an external time dependent force F(t). Here, k is a constant, x, the distance from the origin and t is the time. At some time T, when the particle has zero velocity at x = 0, the external force is removed. The particle will
A system of four particles is in X-Y plane of these two particles of masses m are located at (1, 1) and (-1, 1). The remaining two particles each of mass 2m are located at (1, 1) and (-1, -1). The xy component of moment of inertia tensor of the system of particles is
A particle of mass m is constrained to move on the plane curve xy = c (c > 0) under gravity (Y-axis vertical). The Lagrangian of the particle is given by
A heavy symmetrical top is rotating about its own axis of symmetry (Z-axis). If I1,I2 and I3 are the principal moments of inertia along X, Y and Z axes respectively then
A particle of mass M moving in a straight line with speed v collides with a stationary particle of the same mass. In the centre of mass coordinate system, the first particle is deflected by 90°. The speed of second particle after collision in laboratory system will be
A car is moving with constant linear acceleration a along horizontal X-axis. A solid sphere of mass M and radius R is found rolling without slipping on the horizontal floor of the car in the same direction as seen from an inertial frame outside the car. The acceleration of the sphere in the inertia frame is
A rod of length L0 makes an angle θ0 with the Y-axis in its rest frame while the rest frame moves to the right along the X-axis with relativistic speed v with respect to lab frame. If γ=(1−c2v2)−21, the angle in the lab frame is
A particle of mass m moves in a potential V(x) = 21 mω2x2 + 21 mμv2, where x is the position coordinate, v is the speed and ω, μ are constants. The canonical momentum of the particle is
A particle of mass 2 kg is moving such that at time t second. Its position in metre is given by r(t)=5i^−2t2j^. The angular momentum of the particle at t = 2 s about the origin in kg-m2/s, is
The Lagrangian of a particle moving in a plane under the influence of central potential is given by L=21m(r˙2=r2θ˙2)−V(r). The generalised momenta corresponding to r and θ are given by
The Lagrangian of a particle of mass m moving in a plane is given by L = 21 [m(vx2 + vy2)] + a(xvy - yvx) where, vx and vy are velocity components and a is constant, The canonical momenta of the particle are given by
Three particles of mass m each situated at x1(t), x2(t) and x3(t) respectively are connected by two spring constants k and unstretched lengths l. The system is free to oscillate only in one-dimension along the straight line joining all the three particles. The Lagrangian of the system is