Lecture Notes: Periodic Motion, Harmonic Motion, and Mass-Spring Systems
Periodic Motion and Simple Harmonic Motion (SHM)
- Periodic Motion: Motion that repeats itself; oscillates back and forth.
- Examples include the mass-spring system and the simple pendulum.
- Mass-Spring System: A spring attached to a mass at a horizontal equilibrium position.
- Restoring Force: A force that pushes or pulls the mass back to the equilibrium position when displaced.
- Hooke’s Law:
F_restore = -kx
k
: Spring constant (newtons per meter)
x
: Distance from the equilibrium position
- The negative sign indicates that the restoring force is always directed opposite to the displacement.
Restoring Force and Spring Constant
- Spring Constant (
k
): Measures stiffness of the spring.
- High
k
: Stiffer spring requiring more force to stretch by a certain length.
- Example: If
k = 100 N/m
, it requires 100 N to stretch the spring by 1 meter.
- Hooke’s Law Explanation: Negative sign is due to restoring force direction.
- At Equilibrium:
F_restore
is zero since x = 0
.
- Practical Examples:
- Stretching a Spring: Force required to stretch a spring can be calculated using
F = kx
.
- Unit Conversion: Use meters for distance to match units of the spring constant.
Work and Energy in Springs
- Work to Stretch a Spring: Work
W = 0.5 kx²
(or potential energy).
- Integral Form: Accounts for variable force.
- Potential Energy (
U
): U = 0.5 kx²
- Mechanical energy is conserved in the absence of friction.
Dynamics of Mass-Spring Systems
- Equilibrium and Motion:
- At Equilibrium: Velocity maximum, restoring force, and acceleration zero.
- Fully Stretched/Compressed: Velocity zero, restoring force, and acceleration maximum.
- Undamped Oscillations: Continue indefinitely in absence of friction.
- Damped Oscillations: Amplitude decreases over time due to friction.
Energy Transfer and Mechanical Energy
- Kinetic Energy (
KE
): KE = 0.5 mv²
- Potential Energy (
PE
): Maximum when stretched/compressed.
- Mechanical Energy (
ME
): ME = KE + PE
, remains constant in frictionless systems.
Acceleration and Velocity Calculations
- Maximum Velocity (
v_max
) and Acceleration:
v_max = (k/m)^{0.5} * A
a_max = (k/m) * A
- Equations can be derived for specific displacements (
x
).
Mathematical Description of SHM
- Position Function:
x = A cos(ωt)
ω = 2πf
where f
is the frequency.
- Velocity and Acceleration Functions:
v(t) = -v_max sin(ωt)
a(t) = -a_max cos(ωt)
Frequency and Period
- Period (
T
): Time to complete one cycle.
- Frequency (
f
): Cycles per second (Hz
).
- Relations:
- Period depends on mass (
m
) and spring constant (k
): T = 2π (m/k)^{0.5}
.
- Higher mass increases period; higher spring constant decreases period.
Practical Problems and Calculations
- Various situations provided to calculate force, compression/stretch distances, energy, velocities, and spring constants.
- Examples include forces required to stretch/compress springs and system responses to changes in mass or spring constant.
Damped Harmonic Motion
- Types: Underdampened, overdampened, and critically damped systems.
- Graphical Representation:
- Non-damped: Constant amplitude oscillations.
- Damped: Reducing amplitude over time.
- Critical Damping: Rapid return to equilibrium without overshooting.
Resonant Frequency
- Resonance occurs when the applied force frequency matches the system’s natural frequency, maximizing amplitude increase.
- Real-world example: Child on a swing.
Practice Problems Covered
- Force required to stretch a spring.
- Compression calculations.
- Effect of changing mass/spring constant on period and frequency.
- Calculating maximum acceleration, velocity, and potential energy.
- Examining periodic motion and energy transformations.
- Equations for SHM in terms of sine and cosine functions.
- Frequency of vibration calculations for different scenarios.
Summary: This lecture provided detailed information on SHM and periodic motion, focusing on the dynamics of a mass-spring system, energy transformations, and the mathematical equations governing these motions.