A) Torque B) Velocity C) Momentum 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) Momentum B) Gravitational potential energy C) Kinetic energy D) Mechanical 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 zero momentum B) The object must have constant velocity C) The net force and net torque acting on the object are both zero D) The object must be at rest
A) Mass of the bob B) Initial velocity C) Angle of release D) Length of the pendulum
A) E = mc2 B) p = mv 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) New physics or a more general framework than Newtonian mechanics. B) Applications in chaos theory. C) The concept of scalar quantities. D) A new set of physical laws.
A) 2N B) 3N C) 4N D) N
A) Constraints B) Generalized velocities C) Cartesian velocities D) Degrees of freedom
A) Potential energy B) Generalized coordinates qr C) Lagrangian density D) Each acceleration ak
A) Static. B) Rheonomic. C) Holonomic. D) Scleronomic.
A) Degrees of freedom B) Generalized coordinates C) Curvilinear coordinates D) Cartesian coordinates
A) Holonomic constraints. B) Rheonomic constraints. C) Scleronomic constraints. D) Non-holonomic constraints.
A) Holonomic constraints. B) Scleronomic constraints. C) Rheonomic constraints. D) Non-holonomic constraints.
A) 1-dimensional real space B) N-dimensional real space C) 3-dimensional imaginary space D) 2-dimensional complex space
A) Dynamic. B) Scleronomic. C) Non-holonomic. D) Rheonomic.
A) Potential energy B) Generalized force C) Kinetic energy D) 4-gradient
A) Classical dynamical variables remain unchanged B) Classical dynamical variables become scalar fields C) Classical dynamical variables are replaced by matrices D) Classical dynamical variables become quantum operators indicated by hats (^)
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) ci (i = 1, 2, 3...) C) xi (i = 1, 2, 3...) D) qi (i = 1, 2, 3...)
A) Euler–Lagrange equations B) Hamilton's equations C) Newton's second law D) Schrodinger's equation
A) momentum line B) Hamiltonian curve C) phase path D) Lagrangian trajectory
A) The action S. B) Hamilton's characteristic function W(q). C) The canonical momentum P. D) The Lagrangian L.
A) Hamiltonian map B) momentum diagram C) configuration space D) phase portrait |