Waves and Oscillations Study Notes

Waves and Oscillations

Basic Reference Information

  • Resource Textbooks:   - Physics for Engineers by Giasuddin Ahmad (Part-1)   - University Physics by Sears, Zemansky, Young & Freedman

  • Compilation Prepared by:   - Dr. Md. Abu Saklayen   - Nipa Roy   - Md. Asaduzzaman

  • Affiliation:   - Institute of Natural Sciences, United International University

  • Online References:   - Web references provided on slides

Basics for Waves and Oscillations

  • Key Topics Covered:   - Differentiation   - Vector Analysis   - Basics of Motion

Derivative Formulas

General Formulas
  1. Definition of Derivative:
       racdudx=extlimho0racf(x+h)f(x)hrac{du}{dx} = ext{lim}_{h o 0} rac{f(x+h) - f(x)}{h}

  2. Derivative of a Constant (k):
       racd(k)dx=0rac{d(k)}{dx} = 0

  3. Derivative of Functions:    - Power Rule:
         racd(xn)dx=nxn1rac{d(x^n)}{dx} = nx^{n-1}    - Constant Times a Function:
         racd(cimesf(x))dx=cimesf(x)rac{d(c imes f(x))}{dx} = c imes f'(x)    - Sum Rule:
         racd(u+v)dx=racdudx+racdvdxrac{d(u + v)}{dx} = rac{du}{dx} + rac{dv}{dx}
       - Difference Rule:
         racd(uv)dx=racdudxracdvdxrac{d(u - v)}{dx} = rac{du}{dx} - rac{dv}{dx}
       - Product Rule:
         racd(uv)dx=uracdvdx+vracdudxrac{d(uv)}{dx} = u rac{dv}{dx} + v rac{du}{dx}
       - Quotient Rule:
         racdracuvdx=racvracdudxuracdvdxv2rac{d rac{u}{v}}{dx} = rac{v rac{du}{dx} - u rac{dv}{dx}}{v^2}    - Trigonometric Derivatives:
         - racddx[extsin(x)]=extcos(x)rac{d}{dx}[ ext{sin}(x)] = ext{cos}(x)      - racddx[extcos(x)]=extsin(x)rac{d}{dx}[ ext{cos}(x)] = - ext{sin}(x)
       - Exponential Rule:
         - racd(bx)dx=bxextln(b)rac{d(b^x)}{dx} = b^x ext{ln}(b)    - Chain Rule:
         - racddx[f(g(x))]=f(g(x))racdgdxrac{d}{dx}[f(g(x))] = f'(g(x)) rac{dg}{dx}

Linear and Rotary Motion

Linear Motion Equations
  1. Position as a Function of Time:    - S=x1+xS = x_1 + x

  2. Velocity and Acceleration
       - v=racx1x0tv = rac{x_1 - x_0}{t}
       - a=racextchangeinvelocityta = rac{ ext{change in velocity}}{t}

  3. Equations of Motion:
       - V1=V0+atV_1 = V_0 + at
       - S=V0t+rac12at2S = V_0 t + rac{1}{2} a t^2

rotary motion equations
  1. Angular Displacement (for rotation):    - θ=θ0+ωt+rac12αt2θ = θ_0 + ωt + rac{1}{2} αt^2
       - ω=ω0+αtω = ω_0 + αt

  2. Centripetal Acceleration:
       - ac=racv2r=ω2ra_c = rac{v^2}{r} = ω^2r

Simple Harmonic Motion (SHM)

Definitions and Characteristics
  • Periodic Motion: Movement that is repeated at constant time intervals (e.g., clock hands, wheels of a car).

  • Oscillatory Motion: A specific periodic motion where an object moves to and from a fixed position (e.g., a pendulum).

  • Simple Harmonic Motion (SHM): A type of oscillatory motion characterized by a restoring force proportional to the negative of the displacement from the equilibrium position.

Equations and Concepts
  • For a system undergoing SHM, the displacement can be represented as:   - x=Aextsin(ωt+φ)x = A ext{sin(ωt + φ)}   - Amplitude (A): Maximum displacement from equilibrium.   - Period (T): The time taken for one complete cycle of the motion.   - Frequency (f): Number of cycles per unit time, defined as
        f=rac1Tf = rac{1}{T}

  • Graphical Representation of SHM: Displays changes in position, velocity, and acceleration over time.

Mass-Spring System in SHM

Hooke’s Law
  • Hooke's Law states that the restoring force (F) is proportional to the displacement (x) from the equilibrium position:   - F=kxF = -kx   - Where k is the spring constant, with units of N/m, indicating the stiffness of the spring.

Energy Considerations in SHM
  1. Kinetic Energy (KE):
       - KE=rac12mv2KE = rac{1}{2}mv^2

  2. Potential Energy (PE):
       - PE=rac12kx2PE = rac{1}{2}kx^2

  3. Total Energy (E):
       - Total mechanical energy in an ideal mass-spring system is constant:    - E=KE+PE=extconstantE = KE + PE = ext{constant}

Sample Problems

  1. Problem Example: A block of mass (m = 0.42 kg) attached to a spring (stretched by 2.1 cm) experiences an acceleration of 9.0 m/s² when released. Determine the spring constant.    - Solution:
       - Using Hooke’s law, calculate:
         k=racmax=rac0.42imes9.00.021=180extN/mk = rac{ma}{x} = rac{0.42 imes 9.0}{0.021} = 180 ext{ N/m}

  2. Energy Calculations: Given k = 19.6 N/m and A = 0.100 m, calculate various energy states, total energy, and velocity at specific displacements.    - a) Total Energy:
         - E=rac12kA2=rac12imes19.6imes(0.1)2=9.8imes102extJE = rac{1}{2} k A^2 = rac{1}{2} imes 19.6 imes (0.1)^2 = 9.8 imes 10^{-2} ext{ J}

  3. SHM of a Loudspeaker: Given amplitude and frequency, find maximum speed of the diaphragm, location of maximum speed.
       - Formula to derive maximum speed ( ext{max}):
         Vextmax=AωV_{ ext{max}} = Aω

Pendulum Motion and Energy

  1. Simple Pendulum: Describes motion where restoring force is provided by gravity.    - The period of a simple pendulum is given by:      T=2extπracextlgT = 2 ext{π} rac{ ext{l}}{g}
       - Where l is the length of the pendulum and g is the acceleration due to gravity.

Damped Oscillations

Definition
  • Damped harmonic motion refers to cases where oscillations decay due to frictional forces, resulting in a gradual decrease of amplitude over time until the motion stops.

Equations
  • The equation governing damped motion incorporates damping constant (b):   mracd2xdt2+bracdxdt+kx=0m rac{d^2x}{dt^2} + b rac{dx}{dt} + kx = 0

LC Circuit in SHM

  1. Overview:    - An LC circuit consists of an inductor (L) and capacitor (C), can exhibit SHM characteristics.

  2. Equations in LC Circuits:
       - The governing equation for the oscillation in LC circuits is analogous to that of SHM:    - racd2Qdt2+rac1LCQ=0rac{d^2Q}{dt^2} + rac{1}{LC}Q = 0    - Where Q is the charge on the capacitor.

Additional Topics

  • Resonant frequencies of circuits and related SHM.

  • Characteristics of different types of damping - underdamped, critically damped, and overdamped motions.

Practice Questions

  1. Analyze parameters of damped oscillations using provided m=400 gm, k=100 N/m, b=45 gm/s to determine conditions and behavior exhibited in oscillatory motion.

  2. Derive complete solutions for oscillating systems under various damping conditions.