Relativity
1. The Speed of Light & Ether Hypothesis
Historical Measurements of \(c\) (\(c = \frac{\Delta L}{\Delta t}\))
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Galileo (1638): Attempted to measure \(c\) using lanterns over a distance \(L\), finding the time delay practically zero for \(L \le\) 1 mile.
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Based on modern values, Galileo's expected delay was \(\approx 10^{-5}\) s, which is too fast for human reaction times.
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Ole Rømer (1644–1710): Studied Jupiter's moon Io (orbital period \(\approx\) 42h) and proved \(c\) is finite by observing eclipse periods shorten or lengthen due to the Doppler effect as Earth moved.
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James Bradley (1729): Used stellar aberration (\(\tan\theta = \frac{v}{c}\)) to calculate \(c \approx 3.01 \times 10^8\) m/s, yielding a 0.4% error.
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Léon Foucault (1862): Bounced light off a rotating mirror over distance \(h\) and used \(c = \frac{2\omega h}{\theta}\) to find \(c \approx 2.98 \times 10^8\) m/s (0.6% error).
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Albert Michelson (1926): Improved Foucault's apparatus with a larger distance (\(h \approx\) 35 km) to refine \(c\) to \(2.99796 \times 10^8\) m/s, dropping the error to 0.001%.
The Ether Paradox
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Visible light is an electromagnetic wave with wavelengths from 400 nm (Violet) to 700 nm (Red) and frequencies from \(7.5 \times 10^{14}\) Hz to \(4.3 \times 10^{14}\) Hz.
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The "luminiferous aether" was a hypothesized space-filling medium for light, but a transverse wave traveling at \(c\) would require an impossibly hard medium, contradicting planetary motion.
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Fizeau Experiment (1851): Measured light in moving water and found a partial ether drag factor of \((1 - \frac{1}{n^2}) \approx\) 0.44.
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Michelson-Morley Experiment (1887): Failed to detect an ether wind (expected 0.4 fringes drift, yielded \(\le\) 0.01 fringes), implying complete ether drag.
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The direct contradiction between Fizeau (partial drag) and Michelson-Morley (complete drag) proved the ether hypothesis was self-contradicting.
2. Special Relativity: Kinematics
Einstein's Postulates & Lorentz Transformation
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Alväger et al. (1964) proved that photons emitted from Pion particles moving at \(v \sim 0.99c\) still travel at precisely \(c\).
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Relativity Principle: Physical laws are identical in all inertial frames, rendering a static ether unnecessary.
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Invariance of \(c\): The speed of light is identical in all inertial frames, regardless of relative motion.
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Standard Transformation from track frame \(K\) to moving train frame \(K'\) uses factor \(\gamma = \frac{1}{\sqrt{1-\beta^2}}\) where \(\beta = v/c\).
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Position transformations: \(x' = \frac{x - vt}{\sqrt{1 - v^2/c^2}}\), \(y' = y\), \(z' = z\).
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Time transformation: \(t' = \frac{t - \frac{v}{c^2}x}{\sqrt{1 - v^2/c^2}}\). \(t' = \gamma(t - \frac{v}{c^2}x)\), \(t = \gamma(t' + \frac{v}{c^2}x')\)
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Relativistic Velocity Addition generalizes to \(w = \frac{u + v}{1 + \frac{uv}{c^2}}\), proving that if \(u=c\), the combined speed \(w\) remains strictly \(c\).
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\(\Phi = kx-\omega t\) is constant in any inertial frames
Time Dilation & Length Contraction
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Relativity of Simultaneity: Events simultaneous in one frame project to different times in another frame via \(T = \frac{v}{c^2}D\), where \(D\) is spatial difference.
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Proper Length (\(L_0\)): Length measured at rest; moving objects experience Length Contraction (\(L = \gamma^{-1} L_0\)).
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Proper Time (\(\Delta t_0\)): Time measured by a single clock at rest; moving clocks experience Time Dilation (\(\Delta t = \gamma \Delta t_0\)).
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Muon Decay Application: Muons traveling at \(v = 0.98c\) have a proper half-life of \(1.52\ \mu\text{s}\).
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To an Earth observer, the muon's time dilates (\(t_{1/2} \approx 7.6\ \mu\text{s}\)); to the muon, the atmosphere's length contracts (from 2000 m to \(\approx\) 398 m).
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Both frames mathematically agree on a 54% survival rate reaching the surface.
Minkowski Space & The Invariant Interval
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The spacetime interval is mathematically invariant across all frames: \(s^2 \equiv (ct)^2 - x^2 - y^2 - z^2\).
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Timelike Separation (\(s^2 > 0\)): Events inside the light cone connectable by sub-light travel, defining Proper Time (\(\Delta t_0 = s/c\)).
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Spacelike Separation (\(s^2 < 0\)): Events outside the light cone, cannot influence each other, defining Proper Length (\(L_0 = \sqrt{-s^2}\)).
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Lightlike Separation (\(s^2 = 0\)): Events exactly on the light cone, connected only by massless particles.
3. Special Relativity: Dynamics
Energy, Momentum & Mass Equivalence
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Relativistic Momentum: \(\vec{p} = \frac{m_0}{\sqrt{1 - v^2/c^2}} \vec{v}\) modifies classical mechanics to preserve momentum conservation in all frames.
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Newton's second law (\(\vec{F} = m\vec{a}\)) is invalid; Force must be defined as \(\vec{F} = \frac{d\vec{p}}{dt}\).
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Rest Energy: \(E_0 = m_0 c^2\).
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Total Energy: \(E = \frac{m_0}{\sqrt{1 - (v/c)^2}} c^2\).
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Kinetic Energy: \(E_k = m c^2 - m_0 c^2\).
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Energy and Momentum unify into a 4-Vector with an invariant magnitude: \(\left( \frac{E}{c} \right)^2 - p^2 = m_0^2 c^2\) / \(E^2 = (pc)^2 + (m_0 c^2)^2\).
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\(v = \frac{p c^2}{E}\)
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Mass-Energy Equivalence (\(E = mc^2\)): Confirmed by Uranium-235 fission, where a mass defect of \(\approx 3 \times 10^{-28}\) kg releases \(\approx 1.6 \times 10^{13}\) J per mole.
The Twin Paradox
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Scenario: Twin A stays on Earth; Twin B travels to \(\alpha\)-Centauri at \(v = 0.8c\).
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Resolution via Frame Shifts: Twin B must accelerate to turn around, instantaneously jumping inertial frames, which shifts the line of simultaneity and accounts for Twin A's rapid aging.
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Resolution via Doppler Effect: Using \(f = \sqrt{\frac{1 \mp v/c}{1 \pm v/c}} f_0\), both twins count physical light signals emitted yearly.
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Twin B receives signals for 3 years redshifted and 3 years blueshifted (totaling 6 years).
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Twin A (Earth) receives redshifted signals for 9 years and blueshifted for 1 year (totaling 10 years), providing perfect observational agreement without paradox.
4. General Relativity
Core Principles & The Equivalence Principle
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General Relativity defines gravity not as a force, but as the curvature of space and time.
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Principle of Equivalence: Gravitational mass (\(m_g\)) is strictly equal to Inertial mass (\(m_i\)).
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An arbitrary gravitational field is physically equivalent to an accelerated reference frame at any local space-time point.
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Predictions & Evidence
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Light Deflection: Light traveling through an accelerating elevator (or gravitational field) bends downward.
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Starlight grazing the Sun deflects by \(\Delta\theta = \frac{4GM_{\odot}}{R_{\odot}}\), which equals 1.75'' arcseconds and was confirmed by Eddington in 1919.
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Gravitational Time Dilation: Clocks deeper in a gravitational potential \(\varphi\) run slower according to \(\Delta t = \frac{\Delta t_0}{\sqrt{1 + 2\varphi/c^2}}\).
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GPS Navigation: Requires constant correction because satellite clocks lose 7 μs/day (Special Relativity velocity effect) but gain 46 μs/day (General Relativity weak gravity effect).
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Gravitational Redshift: Photons expend energy to escape massive objects, increasing their period and decreasing their frequency \(\nu\).
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Spacetime curvature governs matter, evidenced by light following null geodesics, Mercury's perihelion precession, and LIGO's 2016 detection of Gravitational Waves.
Thermal Physics
1. Fundamental Thermodynamic Concepts & Temperature
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Thermodynamic Systems: Macroscopic bodies separated from surroundings; classified as Open (exchanges energy and matter), Closed (exchanges only energy), or Isolated (exchanges neither).
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Thermal Equilibrium: A state where macroscopic properties do not change with time, though microscopic properties remain dynamic.
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The Zeroth Law: If systems A and B are each in thermal equilibrium with system C, they are in thermal equilibrium with each other.
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Absolute Temperature: Gases at constant volume extrapolate to zero pressure at -273.15°C. The Kelvin scale conversion is \(T^{(C)} = T^{(K)} - 273.15\).
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Thermal Expansion: Linear expansion is \(\Delta L = \alpha L_0 \Delta T\) and volume expansion is \(\Delta V = \beta V_0 \Delta T\), where \(\beta = 3\alpha\).
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Water's Expansion Anomaly: Between 0°C and 4°C, water has \(\beta < 0\), meaning it contracts when heated and reaches maximum density at 4°C.
2. Heat & Transport Phenomena
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Heat Capacity (\(C\)): Dictates temperature change upon absorbing heat: \(C = \frac{\Delta Q}{\Delta T}\).
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Latent Heat (\(L\)): Heat required for a phase transition where temperature remains constant, calculated as \(Q = LM\).
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Fourier's Law of Heat Conduction: Heat current \(j_q = -k \frac{dT}{dx}\), where \(k\) is thermal conductivity and the negative sign indicates heat flows opposite to the temperature gradient.
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Mean Free Path (\(l\)): Average distance traveled between molecular collisions: \(l = \frac{1}{\sqrt{2} \pi d^2 (N/V)}\) or \(l = \frac{k_B T}{\sqrt{2} \pi d^2 p}\) for ideal gases.
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Microscopic Thermal Conductivity: Derived as \(k = \frac{1}{3} \rho \overline{v} l c_v\).
3. Kinetic Theory of Gases
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Ideal Gas Law: \(PV = nRT\) or \(PV = N k_B T\).
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Van der Waals Equation (Real Gas): \((P + \frac{aN^2}{V^2})(V - Nb) = N k_B T\), where \(a\) corrects for intermolecular forces and \(b\) corrects for molecular volume.
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Kinetic Derivation of Pressure: \(P = \frac{n N_A m}{3V} \overline{v^2}\).
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Equipartition Theorem: The average kinetic energy per degree of freedom is \(\frac{1}{2}k_B T\) per molecule. Degrees of freedom (\(f\)) equals \(t + r + 2s\) (translational + rotational + 2 \(\times\) vibrational).
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Internal Energy (Monoatomic Ideal Gas): \(U = \frac{3}{2} n R T\).
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Molar Heat Capacities: Constant volume \(C_V = \frac{1}{n}\left(\frac{dU}{dT}\right)_V\) and constant pressure \(C_P = C_V + R\) (Mayer's relation).
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Maxwell Velocity Distribution characteristic speeds: Order is \(v_p < \overline{v} < v_{rms}\).
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Most Probable Speed (\(v_p\)): \(v_p = \sqrt{\frac{2 k_B T}{m}}\).
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Average Speed (\(\overline{v}\)): \(\overline{v} = \sqrt{\frac{8 k_B T}{\pi m}}\).
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Root-Mean-Square Speed (\(v_{rms}\)): \(v_{rms} = \sqrt{\frac{3 k_B T}{m}}\).
4. The First Law of Thermodynamics
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First Law Equation: \(\Delta U = \Delta Q - W\), or in differential form, \(dU = \delta Q - \delta W\).
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Work Done (\(W\)): \(W = \int P dV\), representing the path-dependent area under a P-V curve.
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Quasi-static Processes: Isobaric (constant \(P\)), Isochoric (constant \(V\)), Isothermal (constant \(T\)), and Adiabatic (\(Q = 0\)).
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Adiabatic Process Relation: \(P V^\gamma = \text{constant}\), where \(\gamma = \frac{C_P}{C_V}\). \(\Rightarrow\) \(T V^{\gamma-1} = \text{constant}\) for ideal gases.
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Heat Engine Efficiency: \(\varepsilon = 1 - \frac{Q_L}{Q_H}\).
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Otto Cycle (Petrol): Uses isochoric heat absorption/rejection. Efficiency is \(\varepsilon_{\text{Otto}} = 1 - \left(\frac{V_2}{V_1}\right)^{\gamma-1}\).
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Diesel Cycle: Uses isobaric heat absorption and isochoric heat rejection.
5. The Second Law of Thermodynamics
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Carnot Cycle: Reversible cycle consisting of two isothermal and two adiabatic processes.
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Carnot Efficiency: \(\varepsilon_{\text{Carnot}} = 1 - \frac{T_L}{T_H}\).
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Refrigerator (Reverse Carnot) COP: \(\varepsilon^{(r)} = \frac{Q_L}{W} = \frac{T_L}{T_H - T_L}\).
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Clausius Statement: Heat cannot spontaneously flow from cold to hot without external work.
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Kelvin-Planck Statement: A cyclic heat engine cannot completely convert absorbed heat into work without rejecting some heat.
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Carnot's Theorem: No irreversible engine can be more efficient than a reversible (Carnot) engine operating between the same reservoirs (\(\varepsilon_I \leq \varepsilon_{\text{Carnot}}\)).
6. Entropy & The Third Law
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Clausius Inequality: \(\oint \frac{\delta Q}{T} \leq 0\), where equality holds only for reversible processes.
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Entropy Definition (\(S\)): A state function defined by the exact differential \(dS = \frac{\delta Q}{T}\) for a reversible path.
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Second Law (Entropy Statement): For any isolated system, \(\Delta S \geq 0\) (entropy never decreases).
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Ideal Gas Entropy Change: \(S = S_0 + n C_V \ln\frac{T}{T_0} + nR \ln\frac{V}{V_0}\).
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T-S Diagrams: Area under a T-S curve represents the total heat transferred (\(Q = \int T dS\)).
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Third Law (Nernst Statement): As \(T \to 0\), the change in entropy for an isothermal process approaches zero (\(\lim_{T \to 0} \Delta S = 0\)).
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Unattainability Principle: It is impossible to reduce a system's temperature to absolute zero in a finite number of steps.
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Boltzmann's Entropy (Statistical): \(S = k_B \ln W\), where \(W\) is multiplicity (number of microscopic configurations).
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Stirling's Approximation: For large \(N\), \(\ln N! \approx N \ln N - N\), used to prove macroscopic entropy from statistical mechanics.