A) Acceleration B) Momentum C) Velocity D) Torque
A) The definition of potential energy B) The relationship between torque and angular acceleration C) The force required to keep an object moving at a constant speed D) The work done on an object is equal to its change in kinetic energy
A) Kinetic energy B) Gravitational potential energy C) Momentum D) Mechanical energy
A) α = Δω / Δt B) a = Δv / Δt C) F = ma D) T = Fd
A) For every action, there is an equal and opposite reaction B) An object at rest stays at rest C) Force equals mass times acceleration D) Energy is always conserved
A) The object must have constant velocity B) The net force and net torque acting on the object are both zero C) The object must be at rest D) The object must have zero momentum
A) Initial velocity B) Angle of release C) Mass of the bob D) Length of the pendulum
A) W = Fd B) E = mc2 C) F = ma D) p = mv
A) It decreases B) It is not conserved and is converted into other forms of energy, such as thermal energy C) It remains constant D) It increases
A) A new set of physical laws. B) Applications in chaos theory. C) The concept of scalar quantities. D) New physics or a more general framework than Newtonian mechanics.
A) N B) 2N C) 4N D) 3N
A) Degrees of freedom B) Constraints C) Generalized velocities D) Cartesian velocities
A) Potential energy B) Each acceleration ak C) Lagrangian density D) Generalized coordinates qr
A) Rheonomic. B) Static. C) Scleronomic. D) Holonomic.
A) Curvilinear coordinates B) Degrees of freedom C) Generalized coordinates D) Cartesian coordinates
A) Rheonomic constraints. B) Holonomic constraints. C) Non-holonomic constraints. D) Scleronomic constraints.
A) Holonomic constraints. B) Rheonomic constraints. C) Scleronomic constraints. D) Non-holonomic constraints.
A) N-dimensional real space B) 3-dimensional imaginary space C) 1-dimensional real space D) 2-dimensional complex space
A) Non-holonomic. B) Dynamic. C) Scleronomic. D) Rheonomic.
A) Generalized force B) Kinetic energy C) Potential energy D) 4-gradient
A) Classical dynamical variables become scalar fields B) Classical dynamical variables are replaced by matrices C) Classical dynamical variables become quantum operators indicated by hats (^) D) Classical dynamical variables remain unchanged
A) N B) Depends on the constraints applied C) 3, regardless of N D) The same as the number of curvilinear coordinates
A) ri (i = 1, 2, 3...) B) xi (i = 1, 2, 3...) C) ci (i = 1, 2, 3...) D) qi (i = 1, 2, 3...)
A) Hamilton's equations B) Euler–Lagrange equations C) Newton's second law D) Schrodinger's equation
A) phase path B) Hamiltonian curve C) Lagrangian trajectory D) momentum line
A) The Lagrangian L. B) The canonical momentum P. C) Hamilton's characteristic function W(q). D) The action S.
A) configuration space B) Hamiltonian map C) momentum diagram D) phase portrait |