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