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