coulombs or esu charge. It s mass is about 1/1837 times the mass of hydrogen atom. Thus mass of electron is

Similar documents
They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.

Physics 2D Lecture Slides Lecture 14: Feb 3 rd 2004

5.1 The Nuclear Atom

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

How many neutrons does this aluminium atom contain? A 13 B 14 C 27 D 40

Session : Plasmas in Equilibrium

3.1 Atomic Structure and The Periodic Table

(Reference: sections in Silberberg 5 th ed.)

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

Outline. Ionizing Radiation. Introduction. Ionizing radiation

How many neutrino species?

1 of 42. Abbreviated title: [SAP-SVT-Nmsm-g & 137] - Updated on 31 July, 09. Shankar V.Narayanan

Lecture #2: Wave Nature of the Electron and the Internal Structure of an Atom

Bohr type models of the atom give a totally incorrect picture of the atom and are of only historical significance.

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions

1 of 46. Abbreviated title: [SAP-SVT-Nmsm-g & 137] - Updated on 07 Oct, 09. Shankar V.Narayanan

Narayana IIT Academy

NET/JRF, GATE, IIT JAM, JEST, TIFR

Exam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.

MILLIKAN OIL DROP EXPERIMENT

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels

Lecture contents. Density of states Distribution function Statistic of carriers. Intrinsic Extrinsic with no compensation Compensation

Physics of the Interstellar and Intergalactic Medium

Ideal crystal : Regulary ordered point masses connected via harmonic springs

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors

H2 Mathematics Arithmetic & Geometric Series ( )

APPENDIX: STATISTICAL TOOLS

Electromagnetic radiation and steady states of hydrogen atom

Discrete Fourier Transform. Nuno Vasconcelos UCSD

Phys 102 Lecture 25 The quantum mechanical model of light

1985 AP Calculus BC: Section I

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1

Chapter 1 Late 1800 s Several failures of classical (Newtonian) physics discovered

Voltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes

Fermi Gas. separation

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

September 23, Honors Chem Atomic structure.notebook. Atomic Structure

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120

Solid State Device Fundamentals

Probability & Statistics,

ECE594I Notes set 6: Thermal Noise

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

to the SCHRODINGER EQUATION The case of an electron propagating in a crystal lattice

Physics 2D Lecture Slides Lecture 12: Jan 28 th 2004

Discrete Fourier Transform (DFT)

The power of analytical spectroscopy

Chapter 8: Electron Configurations and Periodicity

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

The pn junction: 2 Current vs Voltage (IV) characteristics

Periodic Structures. Filter Design by the Image Parameter Method

The failure of the classical mechanics

07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n

Solution to 1223 The Evil Warden.

Contemporary, atomic, nuclear, and particle physics

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2

Joule-Lenz Energy of Quantum Electron Transitions Compared with the Electromagnetic Emission of Energy

Physics Methods in Art and Archaeology

The real E-k diagram of Si is more complicated (indirect semiconductor). The bottom of E C and top of E V appear for different values of k.

NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011)

Digital Signal Processing, Fall 2006

ECE 340 Lecture 38 : MOS Capacitor I Class Outline:

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

What makes laser light special? Lasers. Lasers. Laser history. Lasers are everywhere! Review of atom discharge lamps. So how do we make laser light?

Title: Vibrational structure of electronic transition

Atomic energy levels. Announcements:

Chapter 4 - The Fourier Series

Hydrogen Atom and One Electron Ions

Structure of the Atom. Thomson s Atomic Model. Knowledge of atoms in Experiments of Geiger and Marsden 2. Experiments of Geiger and Marsden

Atom as a Dressed Nucleus

Circular Array of Tapered Nylon Rod Antennas: A Computational Study

ECEN 5005 Crystals, Nanocrystals and Device Applications Class 14 Group Theory For Crystals

Electronic Supplementary Information

Partition Functions and Ideal Gases

A Simple Proof that e is Irrational

Physics 2D Lecture Slides Lecture 14: Feb 1 st 2005

INTRODUCTION TO SAMPLING DISTRIBUTIONS

Coupled Pendulums. Two normal modes.

Electrochemistry L E O

SPH4U Electric Charges and Electric Fields Mr. LoRusso

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z

Alpha and beta decay equation practice

4E : The Quantum Universe. Lecture 5, April 5 Vivek Sharma

REGISTER!!! The Farmer and the Seeds (a parable of scientific reasoning) Class Updates. The Farmer and the Seeds. The Farmer and the Seeds

A central nucleus. Protons have a positive charge Electrons have a negative charge

PURE MATHEMATICS A-LEVEL PAPER 1

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Bipolar Junction Transistors

Chapter Taylor Theorem Revisited

Solid State Theory Physics 545 Band Theory III

Terahertz band-gap in InAs/GaSb type II superlattices

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Transcription:

1 ATOMIC STRUCTURE Fudamtal Particls: Mai Fudamtal Particl : (a) Elctro: It is a fudamtal particl of a atom which carris a uit gativ charg. It was discovrd by J.J. Thomso (1897) from th studis carrid out o cathod rays i th discharg tub. Wh a high voltag currt (10, 000 volts) is passd btw two lctrods i a discharg tub cotaiig a gas (which is a poor coductor of lctricity) at a vry low prssur (0.01 mm Hg), a stram of gativly chargd particls flow from cathod (mtal rod) to aod. Ths rays wr calld cathod rays & cosistd of stram of gativly chargd particls calld lctros. Proprtis : It is th lightst particl also kow as - particls It carris 1.6 10 19 coulombs or 4.8 10 10 su charg. It s mass is about 1/1837 tims th mass of hydrog atom. Thus mass of lctro is 8 9.1 10 gm or 31 9.1 10 kg or 0.0005486 amu. Th /m ratio of lctro is costat irrspctiv of th atur of th gas & th mtal, usd i discharg tub xprimt. Ratio of /m, as stimatd by Thomso is 8 1.7610 coulombs / gm 0 It is rprstd by 1. 13 Radius of lctro is.8 10 cm. (b) Proto: A atom is lctrically utral ad lctro cotai gativ charg, it follows that a qual magitud of positiv lctricity must also b prst i a atom. Goldsti (1886), wh usd prforatd cathod i discharg tub xprimt foud that i additio to cathod rays, thr ar positiv rays, calld caal rays; movig i th opposit dirctio. By studyig th bhaviours of ths rays i lctro & magtic fild, ths rays wr foud to cosist of havy positivly chargd particls, calld protos. Proprtis: It cotai 1.6 10 19 coulombs or 10 4.8 10 su charg. Th mass of proto is arly qual to that of th hydrog. It is 1.67 10 kg or 4 1.67 10 gm or 1.0078 amu /m ratio for proto dpds o th gas tak i th discharg tub xprimt. /m of proto is 38 9.5810 coulomb/gm Volum of proto is 38 3 1.5 10 cm or uclar dsity is of th ordr of 10 gm/cm 3. (c) Nutro: Chadwick (193) discovrd that wh Bryllium was bombardd by particl, a subatomic particl of mass slightly gratr tha proto & utral i origi obtaid. It is calld utro. It is ot dflctd by lctric ad magtic fild. Proprtis: It has mass 4 1.675 10 gm or 7 1.675 10 kg or 1.00866 amu It is havist particl of a atom. Nutro ad proto rsids at th ctr of atom calld uclus. Nutro ad proto togthr calld as uclos. Nutro ca disitgrat ito proto ad utro. 7 14 H.O.: 8-A/11, Jia Sarai, Nar-IIT, Nw Dlhi-16, Ph : 011-6851008, 6861009 www.carrdavour.i B.O.: 48, First Floor, Mall Road, G.T.B. Nagar (Mtro Gat No. 3), Dlhi-09, Ph: 011-654644, 95409991

Som Ucommo Fudamtal particls: 0 (i) Positro : 1 - It is th positiv coutrpart of lctro, discovrd by Adrso (193). It is vry ustabl ad combis with lctro producig rays (ii) Nutrio: Ths ar discovrd by Paullig (1934) & hav small ( 0) mass ad zro charg. (iii) Atiutrio: Ths wr discovrd by Frmi (1934) & is idtical to utrio but havig opposit spi. (iv) Msos: Ths wr discovrd by Yukawa (1935). Thy may b positivly, gativly or utral. Thir mass is itrmdiat btw that of a lctro ad a proto. Msos Charg Mass / 86 m / / 0 70 m k / / 0 970 m (v) Atiproto: It mass is qual to a proto ad charg is qual to a lctro. (vi) Atutro: It s mass is qual to a utro ad charg is qual to zro. It is idtical to utro but opposit spi. Som Importat Dfiitios: (i) Isotops: Th atoms of a lmt which hav th sam atomic umbrs but diffrt atomic mass. Thy hav sam chmical proprtis but diffrt physical proprtis. Isotops hav diffrt umbr of utros. (i) 16 8 O, 17 8 O,18 8 O (ii) 1 1 H, 3 14 15 1 H, 1H (iii) 7 N, 7 N (ii) Isobars: Diffrt atoms which sam atomic masss but diffrt atomic umbrs. 40 40 40 18 Ar, 19K, 0Ca (iii) Isotos: Thos which cotai sam umbr of utro. 30 31 3 14 Si, 15P, 16S (iv) Isolctroic: Thos atoms or io which hav sam o. of lctros ar kow as isolctroic. 17 Cl, 18 Ar, 19 K, 0 Ca (vi) Isodiaphrs: Th lmt which hav th sam valu of (N P) is calld isodiaphrs. 7 9 11 13 3 Li, 4B, 5 B, 6 C H.O.: 8-A/11, Jia Sarai, Nar-IIT, Nw Dlhi-16, Ph : 011-6851008, 6861009 www.carrdavour.i B.O.: 48, First Floor, Mall Road, G.T.B. Nagar (Mtro Gat No. 3), Dlhi-09, Ph: 011-654644, 95409991

3 Bohr s thory of hydrog atom It dpds upo Max Plack s Quatum thory. Postulats: Nils Bohr (1913) (i) Th lctros travl i orbits that hav discrt quatizd spds & thrfor, quatizd rgis. That is, ot vry orbit is possibl but oly crtai spcific os, at crtai spcific distacs from uclus. (ii) Th lctros do ot cotiuously los rgy as thy travl. Thy ca oly gai & loos rgy by jumpig from o allowd orbit to aothr. (iii) Wh a lctro maks a jump from o orbit to aothr, th rgy diffrc is carrid away (or supplid) by a sigl quatum of light (calld a photo) which has a rgy qual to th rgy diffrc btw two orbit. (iv) Th frqucy of th mittd photo is o ovr th classical orbit priod, corrspodig to th classical missio frqucy. (v) Elctro ca mov oly i thos orbit i which thir agular momtum is a itgral multipl of h/. h i.. mvr Thus agular momtum is quatizd. Applicatio of Bohr s thory: 1. Radius of th orbit: For H ad H lik atoms Li, B h r 4 m whr h = Plack s costat, m = mass of lctro, = charg o lctro = atomic umbr, = orbit umbr O puttig valu of kow costat. r 0.59 Å z. Vlocity of a lctro i th shll: v ; h 8 v.18810 cm / sc 3. Ergy of lctro i th orbit: E 4 m h H.O.: 8-A/11, Jia Sarai, Nar-IIT, Nw Dlhi-16, Ph : 011-6851008, 6861009 www.carrdavour.i B.O.: 48, First Floor, Mall Road, G.T.B. Nagar (Mtro Gat No. 3), Dlhi-09, Ph: 011-654644, 95409991

Pottial rgy Total rgy kitic rgy 19 (i) Total rgy 13.6 V/atom 131 kj/mol.1810 J/atom Ioisatio Ergy: Durig ioisatio a lctro movs from lowst rgy stat to ifiity, whr thr is o forc of attractio ad thus E 0 E E E 1 0 13.6 V/atom ; E 13.6 V/atom Elctromagtic Radiatios: Th radiatios which do ot dviat from lctric ad magtic fild, ad travl i vacuum with spd of light. : Radio wavs, microwavs, X-rays, rays, I.R. UV, visibl ad Cosmic rays. Emissio Spctrum of hydrog: Durig th display of missio spctrum, matrial is radiatd with hat or lctricity, this causs xcitatio of lctro by absorptio of rgy. O rlaxatio this absorbd rgy is lost as light radiatio ad givs missio spctrum. I missio spctrum of hydrog atom, thr ar six typs of missio lis. It ca b xplaid by takig a sampl of hydrog which cotai millios of hydrog atom. Thus diffrt atoms absorb diffrt amout of rgy ad th rlaxs upto diffrt lvl. Thus givs various spctral li. Th wavlgth or wavumbr of light ca b obtaid by rgy diffrc btw two lvls. 4 4 hc m 1 1 ; h 1 Whr, 4 4 m m E.h 1 h 1 1 V R H cm 1 1 1 V = wavumbr; R H = Rydbrg costat (109677 cm 1 ) (E ) E= E - E 1 (E ) 1 1 1 1 V 109677 1 M = 8 = 7 = 6 = 5 = 4 = 3 Pasch Bracktt pfud Humphry I.R. rgio = M = 1 Lyma UV- rgio Balmr visibl rgio H.O.: 8-A/11, Jia Sarai, Nar-IIT, Nw Dlhi-16, Ph : 011-6851008, 6861009 www.carrdavour.i B.O.: 48, First Floor, Mall Road, G.T.B. Nagar (Mtro Gat No. 3), Dlhi-09, Ph: 011-654644, 95409991

(i) For Lyma sris : 1 1,,3,4,5... (ii) For Balmr Sris: 1 ; 3,4,5,6... (iii) For Pasch sris: 1 3 ; 4,5,6,7... ; (iv) For Bracktt sris: 1 4; 5,6,7,8... (v) For pfud Sris: 1 1 V R H 1 1 1 V R H 1 1 V R H 3 1 1 V R H 4 1 5 ; 6,7,8,9 ; 1 1 V R H 5 (vi) For Humphry Sris: 1 1 1 6 ; 7,8,... V R H 6 Not: If a lctro from th xcitd stat coms to various rgy stats, th maximum spctral lis obtaid 1 will b. Limitatios of Bohr s thory: (i) It fails to xplai spctra to atoms with mor tha o lctro. It ca oly xplai th spctra of hydrog ad sigl lctro spcis lik 3 H, Li, B tc. (ii) It dos ot xplai fi structur of spctral lis. (iii) It dos ot xplai ma ffct (Splittig up of spctra lis i prsc of a magtic fild) & stark ffct (splittig up of spctral lis i prsc of a lctric fild) (iv) Fails to rcogis wav proprty of lctro propod by d Brogli. Wav - Particl Duality of Mattr/d-brogli quatio: All th discrt particls of mattr i motio ( lctro, proto, utro, atoms ad molculs) possss particl as wll as wav charactristics, i.. dual charactr is ot oly possssd by radiatio but also by all th microscopic particls of mattr. It mas that a lctro or othr microscopic particl is ithr a particl or a wav. It is a tity which is capabl of dvlopig o of ths faturs dpdig upo th typ of th itractio with xtral world. d-brogli s quatio: From Plack quatio, E hv, c hc E... (1) 5 H.O.: 8-A/11, Jia Sarai, Nar-IIT, Nw Dlhi-16, Ph : 011-6851008, 6861009 www.carrdavour.i B.O.: 48, First Floor, Mall Road, G.T.B. Nagar (Mtro Gat No. 3), Dlhi-09, Ph: 011-654644, 95409991