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