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HIUS 318 notes for Feb 20

Course: HIUS 318 405HH, Spring 2009
School: UVA
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HIUS 318 notes for Feb 13

UVA - HIUS 318 - 405HH

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HIUS 318 notes for Feb 9

UVA - HIUS 318 - 405HH

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HIUS 318 February 11 notes

UVA - HIUS 318 - 405HH

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Week 02 - The Nature and Kinds of Research

University of Toronto - PSYCH - Lab

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The Vertebrates: Structure, Function and Evolution (BIOEE 2740) Lab 3 Chondrichthyes, the cartilaginous fishes.Major concepts The evolution of jaws allowed vertebrates to eat and specialize upon a diversity of foods The evolution of 2 sets of pai

Lab4Osteichthyes

Cornell - BIOEE - 2740

The Vertebrates: Structure, Function and Evolution (BIOEE 2740) Lab 4 Osteichthyes, the bony fishes.Major concepts The two major divisions within the Osteichthyes are the Sarcopterygii, the lobe-finned fishes, and the Actinopterygii, the ray-finne

VertsLab2

Cornell - BIOEE - 2740

The Vertebrates: Structure, Function and Evolution (BIOEE 2740) Lab 2 Invertebrate relatives of the vertebrates and the jawless craniatesGoals for this lab: 1. Learn what morphological features define the major deuterostome groups, and how these gr

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Bentley - SC - 424111

Biological Molecules - 1 Molecules of Living Organisms We have mentioned that all organisms, from bacteria to Douglas fir trees to humans share a common molecular structure; it's part of the unity of life. The cells and tissues of virtually all organ

Cells101

Bentley - SC - 424111

Cell - 1 Just as the atom is the fundamental unit of matter, the cell is the fundamental unit of living organisms. Each cell is unique, composed of carbohydrates, proteins, lipids, and other substances, organized into an orderly structural and functi

Chemistry101

Bentley - SC - 424111

Chemistry Concepts - 1 As indicated in our course introduction, much of Biology 101 emphasizes the study of cells, which structurally and functionally are an aggregate of atoms and molecules (chemicals) working together, and which require the energy

DNATechnology101

Bentley - SC - 424111

Biotechnology - 1 We have discussed some of the ways in which the structure of DNA can be changed in individuals through mutation and how DNA changes from generation to generation through recombination and independent assortment during meiosis and se

Energy101

Bentley - SC - 424111

Energy Flow in Cells - 1 Thousands of chemical reactions occur in our cells and tissues to keep us alive (and hopefully healthy). We have discussed some of the molecules of living organisms (carbohydrates, lipids, proteins, etc.) in the context of th

EvolutionMechanisms101

Bentley - SC - 424111

Evolutionary Mechanisms - 1 The Gene Pool and Genetic Equilibrium As we stated at the beginning of our discussion on evolutionary principles, evolution involves changes that occur in the frequency of a gene's alleles in a population from generation t

EvolutionPrinciples101

Bentley - SC - 424111

Principles of Evolution - 1 We have seen in this course that recombination, segregation of alleles, and independent assortment of homologous chromosomes during meiosis results in the variation that occurs among individuals in populations. We have see

chap1

Bentley - SC - 420112

(Electrostatic)- 2 - - + () q1q2 F 2 r1 4 0q1q2 F =k 2 rk== 8.9875 10 9 N .m 2 / C 2 9 10 9 N .m 2 / C 2 F Fq1q2 F21 = F12 = k 2 r F21 2 1 F12 1

chap2

Bentley - SC - 420112

2 Wa = mgya a bWa = qEy a Wb = qEybWb = mgybW = W f Wi = qE (l f li )W = Wb Wa = qE ( yb ya ) negativeW = Wb Wa = qE ( yb ya ) positiveW = Wb Wa = qE ( yb ya ) positiveW = Wb Wa = qE ( yb ya ) negative

chap3

Bentley - SC - 420112

Q V Q = CVQ C= V Q C= V coulomb = [Farad ] Volt 1 F = 106 F = 1012 pF A EA = = 0 0QQ C= VQ E= A 0V = EdQd E= A 0Q 0 A 0 A = C = Qd d L ra < r < rbr ra rbL E ( 2rL) = = 0 0Qra

chap4

Bentley - SC - 420112

(J) V 1 (junction rule) I = 0I1 = I2 + I3 2 (loop rule) I 3 + - -+ +- + I-+V =05 2 2I 3I 2I = 07I = 33 I = 7 3/7 4 +2 2- + I2 (1) 6 I1 = 4 + 2 I 2I1 =

chap5

Bentley - SC - 420112

P - P - dsR d z 1. 2. 3. 4. vBmv r= qB mv sin = qBvvB s = v/ t= (v cos )tvv B = v sin v/ B = v cos B B2m s = (v cos ) qB 2m t T = qB

chap6

Bentley - SC - 420112

N y x ? 1t dv v0 v = 0dtv exponential . . . . +. . .+ . dr. . .+. . .- -. - - r . . . .- - . . .+ . . . + . R . . . .. +. . . + . . +.

chap8

Bentley - SC - 420112

1. 2. E=Q 4 0 r 2Q2 EdA =4 0 r vvQ E dA = 4r 2(1)vv B dA = 0(2)03.I4.-d B V = N v v dt V = E dlvv vv B dA (3) E dl = t l(4) v E = E ( x, t ) j v B = B ( x, t )k R L L

chap8s

Bentley - SC - 420112

nj1.rrrj 2.nj1rn j n ojn } noEQ 4SH 0 r 2Q 4SH 0 r 2 *Q E dA u 4Sr 2(1)nj EdA B dA**0(2)H0rr3.njnjnjn * E E x, t j *B B ( x , t )krI4.r-rrrnj n or r r r* E dl d) B V N * * dt V E

chap9

Bentley - SC - 420112

=vt AA i BB r AAB BBA AB BA AB iri = r(1 ) OAB IAB OB = IB d o = d i (2 ) C A B OCB IC B OC = IC ho = hi(3 ) 1 1.60 . 10 .E

chap10-ligth

Bentley - SC - 420112

1. 1.1 Youngs Experiment c = 3 = 90 b = 2 a = 1 = d sin = m , m = 0,1, 2, . (1) 1 = d sin = m + , m = 0,1, 2, . (2) 2 m ym = tan m L y m = L tan m tan m sin m my m = L

chap11

Bentley - SC - 420112

11 1. 20 1900 1920 Schrodinger Heisenberg 19 20 2. R = R( )d0 R ( ) 1. 2. T R Rmax shot m 1 T b m = (1) T b = 2.898 10 3 m.K m 3. R = T 4 (2) = 5.67 10 8 W / m 2 K 4 (Wien's Displacemen

chap12

Bentley - SC - 420112

12 Thomson's Plum-pudding Model; J.J. Thomson,1890 Rutherford Rutherford's Planetary model ,1911Gas-discharge tube Hydrogen Balmer series1 1 = R 2 2 ; n = 3, 4, 5, 6, . 2 n R = 1.097 10 4 m 1 Rydberg constant 1Lyman series11

chap13

Bentley - SC - 420112

13 1. - proton = + e = +1.6 10 19 C = 1.6726 10 27 kg - neutron 1.6749 10 27 kg nucleon (atomic number)Z () (atomic mass number)A A Z A ZX X (isotopes) 13C , 14C , 15C , 16C 6 6 6 6 Rutherford4 3 V A V =

chapte13em_waves

Bentley - SC - 420112

Chapter 13 Maxwells Equations and Electromagnetic Waves13.1 The Displacement Current . 2 13.2 Gausss Law for Magnetism .. 4 13.3 Maxwells Equations . 4 13.4 Plane Electromagnetic Waves .. 6 13.4.1 One-Dimensional Wave Equation . 9 13.5 Standing Elec

chapter7

Bentley - SC - 420112

fav f(x) 1 f av = f ( x ) = x2 x1x2 f ( x )dxx1V (t ) = V p sin t1T Vav = V (t ) = 0Vp sin tdt T 0Vp 2 = cos T T t 0T=0 (effective value) (root mean square, rms) V (t ) = V p sin t(V (t ) )2 = Vp 2 sin2 tV2

Chapter_26