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Period (T) is defined as __, and its SI unit is __.
The time taken for one complete cycle of motion; seconds (s)
Frequency (f) is defined as __, and its SI unit is __.
The number of cycles per second; Hertz (Hz)
The mathematical relationship between period and frequency is given by the equation __.
f = \frac{1}{T}
The Hertz (Hz) is defined as __.
One cycle per second.
The maximum displacement from the equilibrium position is called __.
Amplitude (A)
A phase shift (\phi) in the context of SHM equations is used to __.
Indicate the initial angle or displacement in oscillation.
The defining characteristic of Simple Harmonic Motion is that the acceleration is __.
Proportional to the displacement and directed towards the equilibrium position.
For an object on a spring undergoing SHM, the two factors that only affect the period and frequency are and .
Mass (m) of the object and spring constant (k).
In Simple Harmonic Motion, the period and frequency are __ dependent on the amplitude (A).
Not.
The force that acts on a mass attached to a spring obeys and is given by the equation .
Hooke's Law; F = -kx
The generalized equation for position (x(t)) as a function of time for a simple harmonic oscillator is __.
x(t) = A imes ext{cos}(eta t + \phi)
The relationship between angular frequency (\omega) and the period (T) is given by __.
\omega = \frac{2\pi}{T}
The equation for maximum velocity (v{max}) in terms of amplitude (A) and angular frequency (\omega) is ___.
v_{max} = A \omega
The equation for maximum acceleration (a{max}) in terms of amplitude (A) and angular frequency (\omega) is ___.
a_{max} = A \omega^2
The equations for the period (T) and angular frequency (\omega) for a mass on a spring relate to the mass (m) and force constant (k) as follows: and .
T = 2\pi \sqrt{\frac{m}{k}} and \omega = \sqrt{\frac{k}{m}}
The force of gravity (mg) affects a mass oscillating on a vertical spring by __ compared to a horizontal spring.
Adding an additional static force on the spring, which modifies the equilibrium position.
The angular frequency (\omega) or period (T) of a vertical spring system due to gravity, because .
Does not change; the system's motion still follows Hooke's Law and the characteristics of SHM.
The two forms of energy that oscillate in an SHM system are and .
Potential energy (U) and kinetic energy (K).
The general equation for total mechanical energy (E{Total}) of an SHM system is ___.
E_{Total} = U + K
Without dissipative forces, the total energy of the SHM system __.
Remains constant.
The equation for the potential energy (U) stored in a spring is __, and the position generally defined as U=0 is __.
U = \frac{1}{2} k x^2; at the equilibrium position (x=0).
In oscillation, the kinetic energy (K) is maximum at __. The velocity (v) at these points is __.
The equilibrium position; maximum velocity (v_{max}).
In oscillation, the potential energy (U) is maximum at __. The velocity (v) at these points is __.
The maximum displacement; velocity is zero.
The maximum total energy (E{Total}) is expressed in terms of the spring constant (k) and amplitude (A) as follows: ___.
E_{Total} = \frac{1}{2} k A^2
The force (F) is related to the slope of the potential energy graph (U vs. x) as __.
F = -\frac{dU}{dx}
The equation for the magnitude of the velocity (|v|) at any position (x) during SHM using energy conservation is __.
|v| = \sqrt{\frac{2}{m}(E_{Total} - U)}
In the context of the potential energy curve (U vs. x), a stable equilibrium point is defined as __.
A point where a small disturbance results in forces that restore the system to equilibrium.
If disturbed from an unstable equilibrium point, an object __.
Will move further away from the equilibrium position.
If the amplitude (A) of a simple harmonic oscillator is decreased, the and will be affected.
Total energy decreases; maximum velocity decreases.
In the energy transformation of a block-spring system from maximum positive displacement (x=+A) to equilibrium position (x=0), the potential energy and kinetic energy .
Decreases; increases.
The type of motion used to model Simple Harmonic Motion (SHM) is __.
Uniform circular motion.
The physical setup to demonstrate the connection between circular motion and SHM involves __, __, and __.
A peg, a disk, and a lamp.
The part of the uniform circular motion that corresponds to the SHM of an oscillating block is __.
The projection of the point moving in circular motion onto the vertical axis.
In this model, the disk must turn at a constant angular frequency (\omega) that is equal to __ from the oscillating system.
The angular frequency (\omega).
If the disk has a radius r, r represents __ in the context of SHM.
The amplitude (A) of oscillation.
The equation for the position (x(t)) of the shadow as a function of time in the rotating peg model is __.
x(t) = r \cos(\omega t)
The tangential velocity of the peg around the circle for a block on the spring equals to __.
The velocity (v) of the block.
The velocity of the shadow is equal to which component of the peg's velocity is __.
The horizontal component.
The equation for the velocity (v) of the shadow (or the SHM object) as a function of time is __.
v = -A \omega \sin(\omega t)
The relationship between the maximum velocity (v{max}) of the SHM object and the radius (A) and angular frequency (\omega) is given by ___.
v_{max} = A \omega
The equation for the acceleration (a) of the shadow (or the SHM object) as a function of time is __.
a = -A \omega^2 \cos(\omega t)
The position equation for the shadow uses \cos(\omega t) because __.
At t=0, the projection starts at maximum displacement (x=+A).
An example of an object that undergoes uniform circular motion is __.
A point on the edge of a rotating wheel.
If the angular speed of the rotating disk is doubled, the period will and the frequency will .
Halve; double.
The two forces acting on the bob of a simple pendulum are and .
Tension in the string; gravitational force.
The small angle approximation is necessary for a simple pendulum because __.
It allows the restoring force to be directly proportional to the displacement.
The equation for the period (T) of a simple pendulum is __.
T = 2\pi \sqrt{\frac{L}{g}}
The period of a simple pendulum is independent of and .
Mass of the bob; amplitude of the swing.
A simple pendulum can measure the acceleration due to gravity (g) by __.
Measuring the period and rearranging the period equation.
A physical pendulum differs from a simple pendulum by __.
Its mass is distributed and not concentrated at a point.
The force of gravity effectively acts on a physical pendulum at __.
The center of mass.
The equation for the period (T) of a physical pendulum is __ in terms of its moment of inertia (I) and the distance from the pivot to the center of mass (L).
T = 2\pi \sqrt{\frac{I}{mgL}}
In the physical pendulum equation, L represents __.
The distance from the pivot point to the center of mass.
The period equation for a physical pendulum reduces to the period equation for a simple pendulum by __.
Assuming that the moment of inertia simplifies under certain conditions.
A torsional pendulum uses __ as a restoring force/torque.
Torsional spring force.
The variable \kappa (kappa) is called and its SI units are .
The torsional constant; N·m/radian.
The equation for the period (T) of a torsional pendulum is __.
T = 2\pi \sqrt{\frac{I}{\kappa}}
The period of a torsional pendulum is dependent on __.
The moment of inertia (I) of the system.
The primary reason real-world oscillations seldom follow true SHM is __.
Dissipative forces such as friction and air resistance.
In damped harmonic motion, the amplitude (A) __ over time.
Decreases.
Non-conservative damping forces remove energy from an oscillating system primarily by __.
Doing work against the motion.
For a system with small damping, the period and frequency __ compared to those of SHM.
Change only slightly.
For small velocity, the mathematical relationship for the damping force (FD) is given by ___.
F_D = -b v, where b is the damping constant.
The differential equation for the net force on a mass undergoing damped harmonic motion is __.
m\frac{d^2x}{dt^2} + b\frac{dx}{dt} + kx = 0
The equation for the position (x(t)) of a damped harmonic oscillator is __.
x(t) = A0 e^{-\frac{b}{2m}t} cos(\omegad t + \phi)
The term A0 e^{-\frac{b}{2m}t} represents ___ in the position equation of a damped harmonic oscillator.
The exponentially decaying amplitude over time.
The equation for the angular frequency (\omega) of a damped harmonic oscillator is given as __.
\omega = \sqrt{\omega_0^2 - \left(\frac{b}{2m}\right)^2}
The natural angular frequency (\omega0) is defined as ___.
\omega_0 = \sqrt{\frac{k}{m}}
The three damping regimes (types of damping) are __, __, and __.
Under damped, critically damped, and over damped.
For a system to be considered underdamped, the mathematical relationship between the damping constant (b), mass (m), and spring constant (k) must be __.
b < 2\sqrt{mk}.
The motion of an underdamped system is characterized by __.
Oscillation with gradually decreasing amplitude.
The condition for a system to be critically damped is when the relationship between damping constant (b), mass (m), and spring constant (k) is __.
b = 2\sqrt{mk}.
The key characteristic of critically damped motion is __, and a common example where it is desirable is __.
The system returns to equilibrium in the least time without oscillating; car shock absorbers.
The motion of an overdamped system is described as __.
Returning to equilibrium without oscillating more slowly than a critically damped system.
There is a maximum value for the damping constant (b) beyond which the angular frequency (\omega) becomes a complex number because __.
Excessive damping occurs, preventing oscillation.
A critically damped system is often desired for car shock absorbers because __.
It brings the system back to equilibrium quickly without oscillation.
Forced oscillations are defined as __.
Oscillations occurring when a periodic driving force is applied to a system.
The natural frequency (\omega0) of a system is defined as ___.
The frequency at which a system oscillates when not subjected to a driving force.
The phenomenon of resonance is defined as __.
The increase in amplitude of oscillation when the driving frequency matches the natural frequency.
For a system to resonate, the driving frequency (\omega) and the natural frequency (\omega0) must be ___.
Equal.
A real-world example of resonance is __.
A swing being pushed at the right time.
The equation for the periodic driving force (Fd) used in the model of forced oscillations is ___.
Fd = F0 ext{cos}(\omega t)
The differential equation for the net force on a mass undergoing forced and damped harmonic motion is __.
m\frac{d^2x}{dt^2} + b\frac{dx}{dt} + kx = F_d
The equation for the amplitude (A) of a forced oscillator's steady-state motion is __.
A = \frac{F0/m}{\sqrt{(\omega0^2 - \omega^2)^2 + (\frac{b}{m}\omega)^2}}
As the driving frequency (\omega) approaches the natural frequency ($\omega0), the denominator in the amplitude equation ___.
Decreases, causing amplitude to increase significantly.
The equation for the maximum amplitude (A{max}) is given as ___, and the relationship between the two frequencies at this point is __.
A{max} = \frac{F0/m}{\frac{b}{m}}; \omega = \omega_0.
The amount of damping (b) affects the maximum amplitude achieved at resonance by __.
Reducing the maximum amplitude as damping increases.
As damping decreases, the width of the resonance curve (amplitude vs. driving frequency) __.
Narrows.
The term used for the narrowness of the resonance curve is __, and this property is desirable in systems like a radio tuner because __.
Quality Factor (Q); it allows for precise tuning to a specific frequency.
The equation for the Quality Factor (Q) is given as __ in terms of natural angular frequency ($\omega_0) and the spread of angular frequency (\Delta\omega).
Q = \frac{\omega_0}{\Delta \omega}
A singer must match the natural frequency of a crystal glass to make it shatter because __.
The glass will resonate and amplify the vibrations until it breaks.
In the forced oscillation system, the motion that occurs before the system reaches its steady-state periodic motion is called __.
Transitional motion.