Introduction to properties of traveling waves.
Transverse Wave: Moves up and down with a speed V; the displacement occurs perpendicular to the direction of wave propagation.
Longitudinal Wave: Moves in push/pull motion with a speed V; the displacement occurs parallel to the direction of wave propagation.
String Wave Speed:
Formula: v_string = ( \sqrt{\frac{T_s}{\mu}} ) where (T_s) is the tension in the string, and (\mu) is the linear mass density.
Speed of Sound:
Formula: v_sound = ( \sqrt{\frac{\gamma k T}{m}} ) where (\gamma) is the specific heat ratio, k is Boltzmann's constant, T is temperature, and m is the mass of the gas molecules.
Wave moves horizontally; string particle moves vertically.
At times t1 and t2, the particle at X1 displaces a distance A_y due to wave motion while maintaining shape.
History Graph: Shows displacement over time.
Amplitude: A, Crest: 2A, Period: T.
Snapshot Graph: Shows wave properties at an instant.
Fundamental relationship for sinusoidal waves: ( v = \lambda f ) where (\lambda = v/f = vT) (T = 1/f).
Sinusoidal wave equation in the x-direction: ( D(x, t) = A \sin(kx - \omega t + \phi_0) )
Where: ( k = \frac{2\pi}{\lambda} ), ( \omega = \frac{2\pi}{T} ).
Reverse the sign for waves traveling in the -x direction.
Sound intensity level in decibels (dB):
Formula: ( \beta = (10 \text{ dB}) \log_{10}(\frac{I}{I_0}) ) where ( I_0 = 1 \times 10^{-12} \text{ W/m}^2 ).
Stationary Observer: Frequencies heard when the sound source moves.
Approaching source: ( f^+ = f_0 \left(1 - \frac{v_s}{v}\right) ).
Receding source: ( f^- = f_0 \left(1 + \frac{v_s}{v}\right) ).
Moving Observers:
Approaching source: ( f^+ = (1 + \frac{v_o}{v}) f_0 ).
Receding source: ( f^- = (1 - \frac{v_o}{v}) f_0 ).
Understanding and using superposition principles in wave mechanics.
Displacement at a point with multiple waves is the sum of individual wave displacements.
The modes of a string correspond to unique wavelengths and frequencies.
Mode number (m): ( \lambda = \frac{2L}{m} ), frequency: ( f_m = \frac{mv}{2L} ).
Pressure variation in air columns with different conditions (open-open, closed-closed, open-closed).
Phase contributions based on path-length differences leading to constructive/destructive interference
- Constructive interference: ( \Delta\phi = 0 ) or integral multiples of ( 2\pi ).
Destructive interference: half-integer multiples of ( 2\pi ).
Circular/spherical waves with in-phase sources lead to patterns of constructive/destructive interference.
General interference condition: ( \Delta\phi = \Delta\phi_0 + \frac{2\pi\Delta r}{\lambda} ).
General case for constructive and destructive: based on path length differences ( \Delta r ).
Characteristics of macroscopic systems to be explored.
Density: ( \rho = \frac{M}{V} )
Pressure: ( P = \frac{F}{A} )
Atomic mass number and Avogadro’s number definitions included.
Kelvin scale defined; 0 K = -273.15 °C, absolute temperature relationship.
Linear expansion proportionality: ( \frac{\Delta L}{L} = \alpha \Delta T )
Volume expansion defined by: ( \frac{\Delta V}{V} = \beta \Delta T )
Written as ( pV = nRT ) or ( pV = Nk_BT )
Where R is the universal gas constant and ( k_B ) is Boltzmann’s constant.
Each point on the p-V diagram represents a unique gas state.
Constant-Volume = isochoric; Constant-Pressure = isobaric process equations detailed.
Defined as isothermal processes, where ( p \propto T )
Energy exchanges in thermal systems focused; conservation lead to first law details.
Integral representation for work done in varying state conditions.
Ideal processes with one term in the first law as zero identified.
Personalization of specific heat definitions and calculations per unit mass or mole.
Distinctions between melting, freezing, and vaporization processes.
Conservation of energy principle in calorimetry problems defined.
Two types of specific heat defined: at constant volume and pressure, with notable relationships.
Rate of heat transfer in materials shown by defined heat transfer equations.
Study topics of thermodynamics expanded to heat engines working principles.
Extraction of heat from reservoirs to perform work and exhaust waste heat.
Efficiency formula identification and its implications for efficiency.
Contrast with heat engines; their efficiency measured by the coefficient of performance.
Steps of the cycle including isothermal and adiabatic processes.
Efficiency of Carnot cycle illustrated with key formulas for both engines and refrigerators.