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terms and definitions from unit 1
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periodic motion
any motion that repeats itself at regular time intervals
period
time to complete one oscillation
frequency
number of events per unit time
oscillation
one complete cycle of periodic motion
simple harmonic motion (SHM)
motion in which the acceleration (and therefore net force) of the system is proportional to the displacement and acts in the opposite direction of the displacement
amplitude
maximum distance of an object from its equilibrium position in SHM
force constant (k)
representation of the stiffness of an object
equilibrium position
rest position for an object in SHM where net force is zero
phase shift
shift of a sine or cosine function left or right along the x-axis
stable equilibrium point
when the forces on both sides of the equilibrium position point towards the equilibrium position, if an object at equilibrium is disturbed, it will return to its equilibrium position
unstable equilibrium point
when the forces on either or both of the sides of the equilibrium position point away from the equilibrium position, if an object at equilibrium is disturbed, it will not return to its equilibrium position
simple pendulum
a point mass (also called a pendulum bob) which is suspended from a string with negligible mass
physical pendulum
any object whose oscillations are similar to those of a simple pendulum, but cannot be modeled as a point mass on a strong
torsional pendulum
a rigid body suspended by a light wire or spring which when twisted oscillates between two maximum angular displacements
natural angular frequency
angular frequency of a mass undergoing SHM
underdamped system
system with a small damping constant (smaller than √4mk), where the amplitude of the motion decays exponentially
critically damped system
system with a damping constant equal to √4mk, where the system asymptotically approaches the equilibrium as quickly as possible without oscillation
overdamped system
system with a large damping constant (larger than √4mk), where the system will approach equilibrium over a longer period of time without oscillation
natural frequency
the frequency at which a system would oscillate if there were no driving and no damping force
resonance
the phenomenon of driving a system with a frequency equal to its natural frequency
transients
the motions of the oscillator forced with a periodic driving force
quality of a system
spread of the angular frequency at half the maximum amplitude divided by the natural frequency
constructive interference
when two waves arrive at the same point exactly in phase; that is, the crests of the two waves are precisely aligned, as are the troughs
destructive interference
when two identical waves arrive at the same point exactly out of phase; that is, precisely aligned crest to trough
fixed boundary condition
when the medium at a boundary is fixed in place so it cannot move
free boundary condition
exists when the medium at the boundary is free to move (not fixed)
intensity
power per unit area
interference
overlap of two or more waves at the same point and time
linear wave equation
equation describing waves that result from a linear restoring force of the medium
longitudinal wave
wave in which the disturbance is parallel to the direction of propagation
mechanical wave
wave that is governed by Newton’s laws and requires a medium
pulse
single disturbance that moves through a medium, transferring energy but not mass
superposition
phenomenon that occurs when two or more waves arrive at the same point
transverse wave
wave in which the disturbance is perpendicular to the direction of propagation
wave
disturbance that moves from its source and carries energy
wave function
mathematical model of the position of particles of the medium
wave number
equal to the ratio of the angle and the position of a periodic function
wave velocity / propagation velocity
velocity at which the disturbance moves
wavelength
distance between adjacent identical parts of a wave
standing wave
wave that, under certain conditions, can bounce back and forth through a particular region, effectively becoming stationary
node
x-positions of a standing wave that are always zero
antinode
x-positions of a standing wave that are alternate between the positive and negative amplitudes
fundamental frequency
frequency driving the first (fundamental, first harmonic) node, the lowest frequency that will produce a standing wave
overtone
all frequencies above the fundamental frequency which produce a standing wave
normal mode
possible standing wave pattern for a string, with normal frequencies
harmonic
resonant frequency that is an integral multiple of the fundamental