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