Fromm Institute for Lifelong Learning University of San Francisco Agenda Modern Physics for Frommies IV The Universe - Small to Large Lecture 1 13 January 2016 Modern Physics IV Lecture 1 48 slides • • • • • 1/48 Administrative Matters Administrative Matters Physics and the Scientific Method Notation and Units Mass vs. Weight Some History; Premodern Physics 13 January 2016 Monday Modern Physics IV Lecture 1 48 slides Tuesday • Lecture Location and Time: Fromm Hall, Broad Room, Wednesdays 1 PM – 2:40 PM Prompt start. • Lecturer: Terrence A. Mulera – HR 114 • Office Hours: TBA and by appointment • Contact Information: 1000 1025___________ 121 L11 1100 ↓ ↓ ↓ ↓ 1210_ _↓_______ 1200 0945_____________ 121 L15 ↓ ↓ ↓ ↓ 1130 __ ↓_______ Friday Saturday Sunday 1300 101 L11 ↓ 210 L11 ↓ 1400 ↓ ↓ ↓ _______↓_______ 1545 ↓ ↓ ↓ _______↓_______ 1545 1500 Modern Physics IV Fromm Institute1 1440 ↓ ↓________ 0955___________ 120 L12 ↓ ↓ ↓ ↓ 1140___↓_______ 210 L13 ↓ ↓ ↓ ↓ _______↓_______ 1545 1600 1700 1800 – e-mail: [email protected] – Phone: (415) 422-5701 Modern Physics IV Lecture 1 48 slides Thursday 0800 0900 13 January 2016 Wednesday 2 1900 1 11 January to 7 March only Preliminary, Updates TBA 3 13 January 2016 Modern Physics IV Lecture 1 48 slides 4 1 Administrative Matters 2 http://modphysicsfrommiies.wiki.usfca.edu/ • Class Wikis – http://modphysfromm4-2016.wiki.usfca.edu/ or link from Fromm web site. • .pdf notes, 4/page posted hopefully night before class. These may change by time of lecture. – Hard copies. How many do we need? • Power Point® slides posted immediately following lecture. Will include any changes to .pdf notes http://modphysfromm2.wiki.usfca.edu http://modphysfromm3.wiki.usfca.edu Please turn off or silence cell phones and pagers. – Material from preceding classes (Albert Einstein’s Universe, The Universe of Schrödinger’s Cat and A Universe of Leptons, Quarks and Bosons) still available at: 13 January 2016 Modern Physics IV Lecture 1 48 slides 5 Thanks for the cartoon to Moose’s, 1652 Stockton St., San Francisco, CA 13 January 2016 Modern Physics IV Lecture 1 48 slides 6 13 January 2016 Modern Physics IV Lecture 1 48 slides 8 Physics and the Scientific Method •Physics is a science -Limited to that which is testable •Concerned with how rather than why •Best defined in terms of the “Scientific Method” •Formulated in the 17th century •Other concerns reserved to Philosophy, Metaphysics and Theology. 13 January 2016 Modern Physics IV Lecture 1 48 slides 7 2 Example: Newtonian Gravitation Observations: Things fall, planets orbit in ellipses etc. Testing: Good agreement with experiment and observation. Measurement of falling objects Celestial mechanics pre-1900 Empirical Law: There is an attractive force between objects which have mass. Refinement of Theory and Further Testing: 1905 – 1920 Theory: Newton’s Law of Gravitation mm F = −G 1 2 2 rˆ r 13 January 2016 Modern Physics IV Lecture 1 48 slides Einstein’s theory of general relativity Eddington’s observation of bending light Precession of Mercury’s orbit 9 13 January 2016 Modern Physics IV Lecture 1 48 slides 10 13 January 2016 Modern Physics IV Lecture 1 48 slides 12 Future Refinement and Testing: Quantum gravity? CAVEAT: A scientific theory can never be proved, it can only be shown to be not incorrect to the limit of our ability to test it. Alternatively, if you cannot devise an experiment which will disprove your conjecture, your conjecture is not science. - Karl Popper (1902-1994) 13 January 2016 Modern Physics IV Lecture 1 48 slides 11 3 Scientific Notation Helen Quinn, What is Science, Physics Today (July 2009) Very large and very small numbers with many zeros before or after the decimal point are inconvenient in calculations. For convenience we write them as Posted on Wiki http://modphysfromm2.wiki.usfca.edu a × 10b 1.0 = 1.0 × 100 e.g. Small to Large: 0.1 = 1.0 × 10 Planck Length: 0.00000000000000000000000000000000001 m . 10.0 = 1.0 × 101 Cosmological Horizon: 150,000,000,000,000,000,000,000,000.0 m ( Anything )0 = 1 −1 0.01 = 1.0 × 10 −2 . 10 −n = 1 10 n 100.0 = 1.0 ×102 13 January 2016 Modern Physics IV Lecture 1 48 slides 13 Results usually presented as 1 digit to left of decimal with exponent adjusted accordingly, i.e. 20 ×102 → 2.0 ×103. 13 January 2016 Modern Physics IV Lecture 1 48 slides 14 Small to Large: Planck Length: 1 x 10-35 m Multiplication: ( a ×10 )( a b1 1 2 Cosmological Horizon: 1.5 x 1026 m × 10b2 ) = a1a2 ×10b1 +b2 ( a ×10 ) = a ( a ×10 ) = b 2 Division: ( a ×10 ) = a ( a ×10 ) a b b1 1 1 b2 2 × 10 b1 −b2 ×102 b a ×10b 2 Cosmological Horizon [units of Planck Lengths (PL)] = 2 Exponents add and/or subtract 13 January 2016 2 1.5 ×10 26 m = 1.5 × 1061 PL 1× 10−35 m/PL 10n 10− n = 1 = 100 = − n n 10 10 Modern Physics IV Lecture 1 48 slides 15 13 January 2016 Modern Physics IV Lecture 1 48 slides 16 4 Mass vs. Weight Units Mass (if non zero) is a measure of the quantity of matter present. Mostly rationalized mks units, i.e. distance in meters, mass in kilograms, time in seconds. e.g. 1 kg of say air corresponds to n molecules of air 2 kg corresponds to 2n molecules Occasional use of cgs units, i.e. centimeters, grams, seconds and of “English” units, i.e. ft., slugs, seconds Mass is independent of the gravitational environment of the matter. 1 kg on Earth = 1 kg on Mars = 1 kg in interstellar space etc. Special units. e.g. light years, parsecs, fermis, barns introduced as needed Alternatively, mass is a measure of an object’s resistance to acceleration. Mass vs. Weight F = ma 13 January 2016 Modern Physics IV Lecture 1 48 slides 17 On Earth's surface 18 Arbitrary definition of “Modern Physics” g = 9.8 m/sec 2 Post 1900 CE Units: kg m/sec2 ≡ Newton (N) Two major foundations Relativity Weight is dependent on the gravitational environment of the object. Weight on Earth ≈ 3 x weight on Mars ≈ 6 x weight on moon. Quantum Mechanics Where were we? Where are we? Maybe we can ask: Where are we going? Common usage: Weights quoted in kg with environment understood to be surface of Earth. Further confusion: lbs. are units of weight, mass units are slugs. 1 slug x (32 ft/sec2) = 1 lb 13 January 2016 Modern Physics IV Lecture 1 48 slides A Brief History of Views of the Universe Weight is a force on an object due to gravity. W = F = mg 13 January 2016 Modern Physics IV Lecture 1 48 slides 19 “It’s difficult to make predictions, especially about the future.” - Yogi Berra 13 January 2016 Modern Physics IV Lecture 1 48 slides 20 5 Socrates → Plato → Aristotle Earth and its place in the universe: geocentric Complex system of interlocking spheres with names like prime mover, cycles and epicycles. The Ancients (mostly Greeks): Physics from the Greek physika meaning “natural things” or the study of nature. All of the ancient civilizations tried to understand their worlds in terms of myths. Anthromorphizication of natural forces e.g. Egyptian sun god, Ra Greek mythology: Zeus, Athena, Aphrodite, Aeres etc. Ca. 600 BC the Pre-Socratics began to apply reason to the comprehension of nature What is the underlying order that is hidden in nature? 13 January 2016 Modern Physics IV Lecture 1 48 slides 21 Aside: A heliocentric theory was proposed as early as the 6th century BC by non other than Pythagoras. . Physical phenomena: 4 elements. Properties and motions of objects could be described in terms of the chemical reaction properties of these elements. Motion: 4 basic types Alteration: Chemical reaction Natural local motion: Weight falling, smoke rising Horizontal or violent motion: Pushing, pulling, throwing Celestial.motion: Involves the interlocking spheres mentioned above. Ptolemaic model. 13 January 2016 Modern Physics IV Lecture 1 48 slides 22 Renaissance: Ca. 1400- 1600 AD The Copernican Revolution Interregnum: Aristotle - Renaissance Not much happening in physics but lots going on in history Observation → Tables of planetary motion Rome dominates the classical world Geocentric (Ptolemaic) model noticeably inaccurate and difficult to calculate. Rome falls ca. 450 AD Dark ages in Europe ca. 450 – 750 AD “ If I had been present at the creation, I would have recommended a simpler design for the universe” Light of classical civilization preserved in Islamic countries. Returned to the West in the Middle ages, 750 – 1350 AD. - Alphonso X (1221 – 1284) Concept of the zero Algebra Anatomy Star charts Pre-Copernican heliocentric theories King of Spain Black Death strikes Europe, 1347 AD, third of population dies 13 January 2016 Modern Physics IV Lecture 1 48 slides 23 13 January 2016 Modern Physics IV Lecture 1 48 slides 24 6 Nicholas Copernicus (1473-1543) Tried a heliocentric model much like that proposed by Aristarchus 1700 years earlier. Model was successful but not overly so. Johanes Kepler (1571 – 1630) Tycho’s assistant. Inherited data base upon Tycho’s death. Assumed orbits were perfect circles, required reintroduction of complexity Elliptical orbits Few converts over 50 years 13 January 2016 Modern Physics IV Lecture 1 48 slides 25 13 January 2016 Modern Physics IV Lecture 1 48 slides 26 T= Galileo Galilei (1564 -1642) 1608: 1st working refracting telescopes a3 M⊙ = 2 T Hans Lippershey, Zacharias Janssen, Jacob Metius in the Netherlands Speculated that some force (like magnetism) originating from the Sun was responsible for planetary motion. 13 January 2016 Modern Physics IV Lecture 1 48 slides Galileo greatly improved design in 1609 27 13 January 2016 Modern Physics IV Lecture 1 48 slides 28 7 Three objections to Kepler’s heliocentric theories: Final nails in the coffin: (1) The Earth cannot move because birds, falling stones etc, would be left behind. The moons of Jupiter, a miniature Solar System Inertia later Newton’s 1st law. Galilean relativity (2) Non circular orbits are contradictory to the non changing perfection of the heavens. CLEA exercise http://modphysfrom m2.wiki.usfca.edu Novae, supernovae, comets already observed Telescopes allowed observation of sunspots, mountains on Moon Observation of the phases of Venus can only be explained in terms of a heliocentric model. (3) No stellar parallax observed. Telescope ⇒ stars are much farther away than Tycho thought 13 January 2016 Modern Physics IV Lecture 1 48 slides 29 Observation of the transit of Mercury across the face of the Sun 13 January 2016 Modern Physics IV Lecture 1 48 slides 30 Newtonian Mechanics (translational) Three laws of motion: This image cannot currently be display ed. 1) A body at rest or in constant rectilinear motion remains at rest or in motion unless acted upon by an outside force. 2) F = ma 3) Momentum is conserved m i vi = m f v f Action - Reaction There are rotational extensions to these laws: e.g. N = I α Sir Isaac Newton (1642-1726) 13 January 2016 Modern Physics IV Lecture 1 48 slides 31 13 January 2016 Modern Physics IV Lecture 1 48 slides 32 8 Angular momentum, L = mvr Triumphs: ( L = r × mv ) This must also be conserved. Careful, it’s a vector so direction as well as magnitude is conserved Li = L f Celestial mechanics, planetary orbits Navigation Mechanical Engineering and the Industrial Revolution Newton’s Law of Gravitation mm F = −G 1 2 2 rˆ r Force acting at a distance 1 force r2 allowed Newton to derive Kepler's Laws. The above Classical Mechanics was accompanied by the 2nd great triumph of pre-20th century physics, Classical Electromagnetic Theory, a.k.a. Classical Electricity and Magnetism, a.k.a. Classical Electrodynamics. Applying the 3 laws of motion with a 13 January 2016 Modern Physics IV Lecture 1 48 slides 33 Ancient Greece, ca. 600 B. C. 34 attraction Rub a rod of amber or hard rubber with a cloth. If you rub various insulators → After rubbing, rod is able to attract small bits of paper or other light material. No real advance in understanding until ca. 1600 A. D. William Gilbert (court physician to Elizabeth I) studied materials that act like amber. repulsion Postulate: There are 2 types of electrical charges like charges repel unlike charges attract Benjamin Franklin: Assign (+) charge to one type and (-) charge to the other. “electric” (elektron is Greek for amber) Electric: modern term is “insulator” Non-electric: “conductor” Modern Physics IV Lecture 1 48 slides Modern Physics IV Lecture 1 48 slides About 100 years later Charles Du Fay showed that there are 2 forms of electrification. Electrical charge 13 January 2016 13 January 2016 Which is ± is arbtrary. Consistent use of a sign convention allows a very concise mathematical formulation of experimental facts. 35 13 January 2016 Modern Physics IV Lecture 1 48 slides 36 9 Coulomb’s Law Franklin’s arbitrary choice: rubbing glass rod w/silk → (+) rubbing amber or hard rubber → (-) Force between 2 charges, q1 and q2 , separated by a distance r 1 q1q2 F= rˆ Another force at a distance. 4πε 0 r 2 Hindsight: Picking signs opposite to Franklin’s choice → more “sensible” conceptual picture. “Hindsight is always 20-20” - .Anonymous ± ↔ ± a ± →← ∓ J. J. Thomson ca. 1900 Discovered the electron. Its charge under the Franklin convention is (-) William Gilbert (1544-1603) 13 January 2016 Modern Physics IV Lecture 1 48 slides 37 13 January 2016 Magnetism: Charles du Fay (1698-1739) Benjamin Franklin (1706-1790) Charles de Coulomb (1736-1806) Modern Physics IV Lecture 1 48 slides 38 Magnetism “The nation that controls magnetism controls the universe. ” Historical: -Diet Smith in Chester Gould’s Dick Tracy, New York Daily News Syndicate (1962) Interactions between ferromagnetic materials (Fe, Ni, Co) Forces of attraction and repulsion Resemble but are quite distinct from electrostatic Use of permanent magnet in Earth’s magnetic field as compass for navigation. In 1819 Ørsted showed connection between electric current and magnetism. Faraday and others, culminating in Maxwell’s equations. 13 January 2016 Modern Physics IV Lecture 1 48 slides 39 13 January 2016 Modern Physics IV Lecture 1 48 slides 40 10 James Clerk Maxwell (1831-1879) Maxwell’s Equations (differential form) ∇ ⋅E = ρ ε0 ∇ ⋅B = 0 ∂B ∇ × E = − ∂t ∇ × B = µ 0 j + µ 0ε 0 ∂E ∂t In traveling wave equation this is 1 ⇒E. M. wave equation ∇ 2 E + µ 0ε 0 13 January 2016 Modern Physics IV Lecture 1 48 slides 41 13 January 2016 ∂ 2E = 0 2 ∂t µ 0ε 0 where ∇2 = Modern Physics IV Lecture 1 48 slides 1 v2 = c = 3 x 10 8 m/sec ∂2 ∂2 ∂2 + + 2 ∂x 2 ∂y 2 ∂z 42 The Deterministic Universe Triumphs: Determinism ⇒ The future is completely determined by the past. ⇒ The future can be predicted if enough is known of the past. Electrical Engineering, Electric power and communication Wireless communication What is enough? Consider a universe whose component objects are labeled with the index i. Each object has mass mi. Radar Modern optics If we know the initial position, xiI, and velocity, viI of each particle plus the resultant or sum of all the forces acting on it as a function of time, Fi(t), then we can, in principle, calculate the final position, xiF, and velocity, viF. , First electronic computers xiI xiF viI Fi(t) 13 January 2016 Modern Physics IV Lecture 1 48 slides 43 13 January 2016 viF Modern Physics IV Lecture 1 48 slides 44 11 Kelvin, Lord William Thomson (1824-1907) “There is nothing new to be discovered in physics now. All that remains is more and more precise measurement.” -1900 “Heavier than air flying machines are impossible.” -1895 “X-rays will prove to be a hoax.” -1896 Lord Kelvin 13 January 2016 Modern Physics IV Lecture 1 48 slides 45 13 January 2016 Modern Physics IV Lecture 1 48 slides Orville Wright Wilbur Wright 1871 - 1948 Wilhelm Röntgen Mrs. Röntgen né Anna Ludwig 1845 - 1923 1872 - 1919 13 January 2016 Modern Physics IV Lecture 1 48 slides 47 13 January 2016 46 1867 - 1912 Modern Physics IV Lecture 1 48 slides 48 12
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