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