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