GEMP 2023 PHYSICS


Outline

  • Physics Reference Materials
  • GEMP Physics Topics
    • Mechanics
    • Properties of matter
    • Elastic & plastic
    • Viscosity
    • Vibrational motion
    • Circular motion
    • Oscillations
    • Resonance
    • Thermodynamics
    • Kinetic theory
    • Real and ideal gases
    • Laws of thermodynamics
    • Electromagnetic Properties of matter
    • Magnetic materials
    • Dielectrics
    • Semiconductors
    • Selected Topics in Modern Physics
    • The photon
    • Heisenberg Uncertainty Principle
    • Particle in a box
    • Selected Measuring instruments
    • Spectrometers

Physics Reference Materials

  • University Physics
  • Fundamentals of Physics
  • Physics: Principles with Applications
  • Sears & Zemansky's University Physics with Modern Physics (Fifteenth Edition, Global Edition)
  • Physics Principles with Applications by Douglas C. Giancoli
  • Fundamentals of Physics by Jearl Walker
  • Halliday & Resnick
  • Previously sold as the 10th Edition
  • Extended

Mechanics

Elastic Properties of Bodies
  • Real bodies deform when stressed.
  • For small deformations, stress is proportional to strain.
    • Stress: extStress=FAext{Stress} = \frac{F}{A}
    • Strain: extStrain=riangleLL<em>0=LL</em>0L0ext{Strain} = \frac{ riangle L}{L<em>0} = \frac{L - L</em>0}{L_0}
    • Young’s Modulus: E=extStressextStrain=FAriangleLL0E = \frac{ ext{Stress}}{ ext{Strain}} = \frac{\frac{F}{A}}{\frac{ riangle L}{L_0}}
Bulk Properties
  • Bulk stress: extBulkstress=FAext{Bulk stress} = \frac{F}{A}
  • Bulk strain: extBulkstrain=riangleVV0ext{Bulk strain} = \frac{ riangle V}{V_0}
  • Bulk modulus: K=rianglePriangleVV0K = -\frac{ riangle P}{\frac{ riangle V}{V_0}}
  • Compressibility: β=1K=1V0riangleVriangleP\beta = \frac{1}{K} = -\frac{1}{V_0} \frac{ riangle V}{ riangle P}
Shear Properties
  • Shear stress: extShearstress=FAext{Shear stress} = \frac{F}{A}
  • Shear strain: extShearstrain=anhetaext{Shear strain} = an{ heta}
  • Shear modulus: G=extShearstressextShearstrainG = \frac{ ext{Shear stress}}{ ext{Shear strain}}
Poisson’s Ratio
  • ν=exttransversestrainextlongitudinalstrain=riangleDD<em>0riangleLL</em>0\nu = -\frac{ ext{transverse strain}}{ ext{longitudinal strain}} = -\frac{\frac{ riangle D}{D<em>0}}{\frac{ riangle L}{L</em>0}}
    • Alternative expressions: <br/>ν=3(12<br/>ν)2(1+<br/>ν)<br />\nu = \frac{3(1-2<br />\nu)}{2(1+<br />\nu)}

Plastic Properties
  • Typical stress-strain diagrams exhibit the following:
    • Elastic limit or yield point: The maximum stress that can be subjected before permanent deformation.
    • Proportional limit: The region of elastic behavior where stress is proportional to strain.
    • Plastic deformation: Permanent deformation occurring after the yield point.
    • Fracture point: The stress where the material finally breaks.
    • Elastic hysteresis: The difference in stress-strain behavior under increasing vs. decreasing stress.

Example: Stress and Strain of an Elongated Rod
  • A steel rod with:
    • Radius: R=9.5extmmR = 9.5 ext{ mm}
    • Length: L=81extcmL = 81 ext{ cm}
    • Force applied: F=62extkNF = 62 ext{ kN}
  • Key ideas:
    1. Stress calculation: extStress=FAext{Stress} = \frac{F}{A} where A = rac{ ext{π}R^2}.
    2. Elongation related to stress and Young's Modulus: riangleL=FLAEriangle L = \frac{F L}{AE} where EE is Young's modulus.
    3. Strain is the ratio of elongation to the initial length: extStrain=riangleLLext{Strain} = \frac{ riangle L}{L}.
Calculations
  1. Compute stress:
    extStress=62imes103Nextπ(9.5imes103m)2=2.2imes108N/m2ext{Stress} = \frac{62 imes 10^3 N}{ ext{π}(9.5 imes 10^{-3 m})^2} = 2.2 imes 10^8 N/m^2

    • The yield strength for structural steel is approximately 2.5imes108N/m22.5 imes 10^8 N/m^2, indicating the rod is near its yield strength.
  2. Young's modulus from table: Esteel=2.0imes1011N/m2E_{steel} = 2.0 imes 10^{11} N/m^2

    • Elongation:
      riangleL=STE=(2.2imes108N/m2)(0.81m)(2.0imes1011N/m2)=0.00089m=0.89mmriangle L = \frac{ST}{E} = \frac{(2.2 imes 10^8 N/m^2)(0.81 m)}{(2.0 imes 10^{11} N/m^2)} = 0.00089 m = 0.89 mm
  3. Strain:
    ext{Strain} = rac{0.00089 m}{0.81 m} = 0.0011 = 0.11 ext{%}


Example: Young's Modulus Calculation
  • Given:
    • Young's modulus = 42 GPa, Poisson ratio: <br/>ν=25<br />\nu = \frac{2}{5}.
  • Find:
    • Bulk modulus: K=3(12<br/>ν)2(1+<br/>ν)=70extGPaK = \frac{3(1-2<br />\nu)}{2(1+<br />\nu)} = 70 ext{ GPa}
    • Shear modulus: G=E2(1+<br/>ν)=15extGPaG = \frac{E}{2(1+<br />\nu)} = 15 ext{ GPa}

Example: Ideal Gas Law
  • State: PV=nRTPV = nRT
  • Isothermal bulk modulus: K=PVnRK = -\frac{PV}{nR},
    • Evaluation under pressure: P = 100 kPa
      ightarrow compressibility = 1/(K) ext{ at temperature T}
Common Problems
  • Biceps Muscle Example:
    • When relaxed requires 25.0 N for elongation of 3.0 cm.
    • Maximum tension requires 500 N for same elongation.
    • Determine Young's modulus for both conditions assuming uniform cylinder properties.

Viscosity
  • Defined as the internal friction in a fluid.
  • Influences and relates flow rate to pressure gradient through the Poiseuille equation.
  • Volume flow rate:
    Q=extvelocityimesextAreaQ = ext{velocity} imes ext{Area}
Example: Water Flow in Capillary Tube
  • Given:
    • Pressure differential: 1.5 mm
    • Viscosity: 0.801 cP.
  • Calculation of water flow in 30 seconds across stated tube diameter:
    Q=5.17imes106m3s1Q = 5.17 imes 10^{-6} m^3 s^{-1}

Vibrational Motion
  • Discussed in context of circular motion with critical acceleration related computations.
  • Centripetal acceleration defined:
    ac=v2ra_c = \frac{v^2}{r}
  • Uniform circular motion is characterized by constant speed and periodic motion.
Example: Kinetic Energy in Circular Motion
  • Object of mass 2kg moving in a circle of radius 20m under centripetal force of 800 N:
    KE=mv22=20mimes800N2=8000JKE = \frac{mv^2}{2} = \frac{20m imes 800N}{2}=8000 J

Resonance
  • Occurs when the driving frequency matches the system's natural frequency.
  • Characterized by motion equations of damped driven oscillators
  • Damping behaviors detail amplitude decay related to system design frequency:
    md2xdt2+bdxdt+kx=0m \frac{d^2x}{dt^2} + b \frac{dx}{dt} + kx = 0

Laws of Thermodynamics
  • Zeroth Law: If system A is in equilibrium with system B, and B is in equilibrium with system C, then A and C are in equilibrium.
  • First Law: riangleU=QWriangle U = Q - W (energy conservation)
  • Second Law: States that all heat cannot be converted into mechanical work without losses.
  • Carnot Efficiency Equation: extEfficiency=1T<em>cT</em>hext{Efficiency} = 1-\frac{T<em>c}{T</em>h}

Real Gases
  • Discuss Van der Waals equation of state and deviations from ideal gas behavior at high pressures or low temperatures.
Example: Ice Melting
  • Determine the energy efficiency when 1 kg of ice melts at 0°C, specific latent heat of ice is 3.34imes105Jkg13.34 imes 10^5 J kg^{-1} resulting in riangleS=1kgimes3.34imes105J273.15Kriangle S = \frac{1kg imes 3.34 imes 10^5 J}{273.15 K}.

Electromagnetic Properties of Materials
  • Discuss magnetic materials, dielectrics, and semiconductors.
Magnetic Properties
  • Diamagnetism: Overall negative magnetization, weakly repelled by external fields.
  • Paramagnetism: Material with unpaired electrons, characterized by a positive weak magnetic susceptibility of about 10410^{-4}.
  • Ferromagnetism: Materials like iron, cobalt, and nickel: strong interactions exist between magnetic dipoles.
    • Magnetization is also dependent on temperature and exhibits hysteresis behaviors.

Semiconductor Properties
  • Discuss intrinsic and extrinsic semiconductors, their band structures, and charge carrier behavior.
Example: Transistor Applications
  • Bipolar junction transistors (BJTs) demonstrate critical current amplification characteristics in circuits.

Selected Topics in Modern Physics
  • The photon is a quantum of the electromagnetic field.
  • Heisenberg Uncertainty Principle: Constraints on precision measurements of conjugate variables.
  • Solve examples related to motion of particles in quantum systems described by the Schrödinger equation.
Example: Mass Spectrometry
  • Explanation of ionized particle dynamics in magnetic fields to quantify masses in atomic units, with specific calculations indicated.