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