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