Balázs HORVÁTH. kábé 10

Size: px
Start display at page:

Download "Balázs HORVÁTH. kábé 10"

Transcription

1 Balázs HOVÁTH káé 10 in eoia E o Alto Saxohone in E-lat and Ha 016 to the Duo Sea AYING SCOE Balázs Hováth, 016

2 káé 10 (cica 10) was coosed in the eoy o the Hungaian wite éte Esteházy in 016 It is dedicated to the Duo Sea (Ezséet Selelo Saxohone and Anasztázia azvalaeva Ha) who equested the iece Howeve the title the iece contains 11 oveents The eason o this is that éte Esteházy entioned that he witing his novel Egy nő (A woen) he wanted to ceate cica 100 sections ut not exactly 100 Theeoe I ceated cica 10 oveents which ae actually 11 The eetitions at the end o the longe oveents ae to e eeated any nue ut stat the eetition at least once I you have to inish togethe agee in a seciic lace o counicate clealy with each othe duing the eoance Duata / Duation: ca -9 in káé 10 was coosed with the inancial hel o the National Cultual Fund, Hungay Wold eiee: /0/01, (H) y Duo Sea (Ezséet Selelo Saxohone and Anasztázia azvalaeva Ha)

3 Secial signs Alto Saxohone in E-lat káé 10 - in eoia E - 01 Quatetone alteation u, down HOVÁTH Balázs (*196) Blow into the intuent using the given inge-key (ooid notehead) ½ Hal (eath) / hal noal sound Oen (had) Sla-tongue (sote sound) Key-clicks with the given keys ite lv 0 ove hand lv gliss gowl 0 (thoat) - lv ± nn tongueinhale STO n n see e = 1 glissando lv gliss ± i inst Ó - no - Ȯ voice coe ia i Ó n n n Multihonic sound with the given itch should doinating o uilt on this itch Gowl with thoat Bite the eed (ute) Highest ossile itch n n lv i nn 1/ 06 hit (ute) 11 glissando hit Inhale, then sto the sound with the tongue Sing and lay siultaneosly 11 Balázs HOVÁTH, 016 Ó lv Ó 1 1/ 1/

4 16 0 INTO I 1 Ha n µ M n Ï F od fio fio ast fi fio on tuning egs g g liss g onthe tuning Glissando egs with lectu (Thow away 1 0 ggg n liss g do down the lectu ate the sound to ulil g ggg this action hit I in the any ties iece, eae 6- lectus, ank cads) g uzz (ute) n fi g away lectu! g e =thow 10 ^ ggg fi µ M Mute at the given oents µ M the sound n INTO n I Ï F F Ï fi fi e = 1 ull e = 10 o eo= 10 e = 1 fio fio vi fio fi on the stings the hand) lace you let hand (edge o sotly and µ 1 9 ull da the (hade olageolet) µ Mhal-lageolet gliss vi n 0 stings Ceate Ÿ than n n hit O sounds Ï F I uzz (ute) fi µ hit ^ (ute) ull M uzz fi fi eod = 10 ast ^ o o µ on tuning "fi " fi fi egs o n g g with sotedal soundn 1 n liss F µotion M fi gggg n Buzz Ï s s ggg n F hit fi0e = 10 gli tongue uzz (ute) Ï gg n STO inhale ull fi 1/ Ÿ thow lectu! 1ast odaway fi gggg sueall ^ n fio fi1/ o ng egs fi o sound oad 9 g (u) gggg n hit ull fi uzz " "gg n(ute) s s see i l ^ hands given hit egiste (ute) and kee you n gggg n n g FHit the stings at aox the uzz ) 10 gg fi e= 1 fi e= 10 thee stong daening way lectu! sound ^ ess ily vi g g µ g Ó M Ÿ Ó fi e =10 ull Ó 9 µ all vi sound gowl n n oad ite ull q =0 - F µ (thoat) Ï coe ia µ inst - so ulleove you hand Osotly 9fi fi that they esonate eove hand o the stings e =1 F n e=o10lv o fi "" n lv ate (You need to kee you hand on the stings the evious ess ily n ull 9 Ó Ó e = 10 hit action you quasi Ó a sot hee ss - Ÿ and n hand eove vi to get voice gli ull esonating esult) hit q = 0 µ uzz (ute)µ - inst edal O- ^ n "" sueall ss ily e= 10 n (u) sound oad the edal should stay at the edal coe ia A E fin ull gliss with uzz sound voice 1/ sueall 1/ aiving (u) - osition (the next alteation always its to - n n µ Ó lv nó this itch) inst F O ess ily sueall oad sound )n (u) ull 9 esueall = 10 Take a sueall (sall ue all this is used yily n ily ess voice ess gowl ull n ite ecussionists) and u the sound oad (Downwad otion is - inst q = 0 n (thoat) µ F O- e 1= 10 ess ess ily ecoended) n ily y n n ull µfi- - inst lv e = 10 fivoice O- ull Ó q = 0 µ - inst Ó n Ó edal n od so O(NO lageolet) ess let hand ily to the stings voice n the n that itches will e quite noisy A esse ily n voice G n n H sueall (u) n n G lv edal H G n ily Ó a A ess A E a n e=10 ess ily ily ess ) ull q = 0 Balázs HOVÁTH, 016 n µ - inst - Balázs HOVÁTH, O ess ily n n G ess ily n ess ily voice lv fi Ó od Ó e = 1 ull e = 10 gliss 9 gliss liss

5 n n n od µ- µ vi vi µ U M sueall 0 (u) lv µǣ inst n O - o U S n F U voice n n Ó Gliss acoss the stings with nail : et it viate lv Ÿ n ˆ 1 n n ess ily n " " tuning key ṗ Ÿ 16 egs n " " π ˆ 1 16 π ess ily Balázs HOVÁTH, 016 AF U lectu ) slow 16 lectu 16 ± 16 ˆ 1 ess ily U 16 lectu 16 1 ˆ ca -6 sec Noal gliss acoss the stings (with lectu) c si (-x) U U hit n (ute) v n n lv i ca -6 sec nn U si (-x) c gliss glissando U U gliss u the given sting with sueall (The diection o the aow will not show the ideal diection you ay u downwads) n ˆ 1 luck the given itch (evis A-natual) ess ily 16 ˆ 1 and lace the tuning Balázs HOVÁTH, 016 Akey at the given lectu itches to lay glissando (Kee the lectu in you hand while lucking so that you can continue the next a) slow 16 F lectu 16 ˆ 1 16 ˆ 1 11 π gliss Scatch the sting lengthwise (with lectu) 16 1 ˆ (Scatch the sting with ingenails O ae tissue twisted aound the sting see ouv 0) u the sting and gliss acoss the stings siultaneously (with sueall) Stat with uwad otion o the soundoad and slide acoss stings only a it late U F inst O - voice n F ite

6 to the Duo Sea káé 10 - in eoia E - 01 INTO ull lectu on tuning egs thow away lectu! ast od I gliss M uzz HOVÁTH Balázs (*196) hit (ute) vi gliss vi "" ull 9 sueall (u) sound oad ess ily gowl (thoat) ite edal C B E sueall (u) lv ess ily ull inst voice ess ily Balázs HOVÁTH, 016

7 Scoe 1 od A G II vi 1 isigl vi glissando E ull sueall (u) sound oad od E D F vi Balázs HOVÁTH, 016 gliss vi M gliss inst ( voice )

8 Scoe III lectu on tuning egs slow : tuning key C "" lectu slow F ess ily lectu E : ess ily lectu od senza sinc senza sinc ca -6 sec si (-x) si (-x) 1 IV a teo C B A G ess ily ess ily Balázs HOVÁTH, 016 lag lag od od

9 od secco ess ily lag od 1 ess ily lag od ess ily lag od V eeat and Fade out (eely) Balázs HOVÁTH, 016

10 6 0 vi n isigl µ vi e = 10 n glissando n gliss M µ vi gliss n Ó o glissando Balázs HOVÁTH, 016

11 Balázs HOVÁTH, 016

12 Scoe INTO ull on tuning egs gliss vi thow away lectu! gliss vi ast od sueall (u) I "" sound oad 0 gliss uzz M ull ess ily hit (ute) 9 1 gowl (thoat) ite edal C B E sueall (u) od lv ess ily H Balázs HOVÁTH, 016 ull inst voice G ess ily D C B E A

13 Scoe 1 II sueall (u) sound oad gowl (thoat) ite lv ull inst voice 9 ess ily F gliss sueall (u) glissando lv 6 III : hit (ute) tuning key C A "" lectu slow B ess ily lectu 1 E : ess ily lectu od senza sinc senza sinc ca -6 sec si (-x) Balázs HOVÁTH, 016

14 10 IV a teo si lectu aízsei/köö "" ast si "" 0 "" "" "" it slow "" "" ast V si "" it slow "" ast 9 slow ast "" slowast "" slow "" ed "" ast "" si "" Balázs HOVÁTH, 016 "" eeat eely then inish the oveent anywhee (togethe) ast slow "" "" "" ast

15 0 11 e = 10 n sueall (u) sound oad gowl (thoat) - ite lv gliss ± nn n n glissando lv hit (ute) i Balázs HOVÁTH, 016

16 1 Balázs HOVÁTH, 016

17 0 1 q = 0 Balázs HOVÁTH, 016

18 1 Balázs HOVÁTH, 016

19 06 1 inst e = 1 - Ȯ voice no- n n n Balázs HOVÁTH, 016

20 16 1 INTO e = ull on tuning egs gliss µ vi n thow away lectu! e = 1 gliss vi µ n ast n n g n od e = 10 i i I e = 10 ḳey-click i o gliss Ÿ " " sueall (u) F sound oad 0 i o i o Ï uzz ^ µ M n hit (ute) i n ull ess ily F 9 gowl (thoat) ite - edal E sueall (u) A lv ess ily n n n q = 0 n e = 10 ull µǣ inst O - voice ess ily 1 a A od n H n G n ṗ Balázs HOVÁTH, 016

21 1 II e = 1 inst - Ȯ voice O - e = 10 ḳey-click e = 1 inst -Ȯ voice µo - e = 10 ḳey-click q = 0 1 n n n i o i o i o n n n i o i o i o e = 10 i o ḳey-click ull ǣ 16 vi n ess ily ull 9 6 inst - Ȯ e = 1 voice O - n n n e = ǣ vi n inst - Ȯ voice ess ily e = 1 O - n n n e = 10 ḳey-click π i o Balázs HOVÁTH, 016

22 1 III e = 10 lectu on tuning egs : n F slow π n n tuning key n n AF Ÿ " " lectu slow π U ess ily lectu 16 ˆ 1 16 ˆ 1 16 ˆ 1 16 ˆ 1 16 ˆ 1 16 ˆ 1 K E K : ess ily lectu Ô sinc ṣenza od ṣenza sinc U U n U U ca -6 sec si (-x) IV 1 a teo Ï Z K F M N B X C V F glissando ull F inst O - voice n F see ite Balázs HOVÁTH, 016

23 19 1 F coe ia O - F coe ia n n coe ia 6 F glissando O - F see no - gliss O F 61 V q = 0 see n n O - glissando n n n n O - O gliss O - n n O - n n 6 O - O - O - O O - gliss gliss n gliss 69 no- O - 9 O O - any itches gliss 9 Balázs HOVÁTH, 016

24 0 0 INTO I e = 1 ull on tuning egs gliss thow away lectu! ast n n g n od i i e = 10 ḳey-click i o gliss i o i o µ M Ï uzz ^ n hit (ute) i F µ vi e = 1 gliss µ vi e = 10 Ÿ " " n ull 9 n n sueall (u) F sound oad ess ily e = 10 gowl (thoat) ite - edal E sueall (u) lv A ess ily n n n q = 0 n ull µǣ inst O - voice ess ily Balázs HOVÁTH, 016

25 1 n ṗ 1 16 a A od H n G n II {q = 60} ull 16 n ǣ 16 nn 16 ˆ 1 - ˆ1 ˆ 1 n n n sueall (u) sound oad q = 0 gowl (thoat) - e = 10 ite lv vi n n ite n ull n ǣ 16 - n n n n q = 0 Balázs HOVÁTH, n 1 n n od µ- n

26 e = 10 III ZG : n n tuning key n n SAU Ÿ " " lectu slow π FY ess ily lectu 16 ˆ 1 16 ˆ 1 16 ˆ 1 16 ˆ 1 16 ˆ 1 16 ˆ 1 K : K E ess ily lectu Ô sinc ṣenza od ṣenza sinc U U n U U ca -6 sec si (-x) IV a teo Ï Z K π H B od π it olto al {e = 90} x = q 6 {e = } (it olto al) {e = 0} q = 0 Ô Balázs HOVÁTH, 016 Ó hit (ute) i Ó see Ó

27 0 e = 10 1/ ( ) Ó Ó eove hand lv inhale tongue- STO see Ó i coe ia Ó 1/ Ó lv Ó ( ) coe ia Ó i Ó 1/ Ó lv 1/ Ó Ṙ Ó i a ( ) Ó lv Ó Ṙ Ó i G 6 Ó V ( ) Ó Ó 1/ lv Ó Ó eeat eely then inish the oveent anywhee (togethe) Ṙ i G : sei-tone highe at each eetition Balázs HOVÁTH, 016

28 09 (INTO) e = 1 ull lectu on tuning egs gliss thow away lectu! ast n n g n od i i Balázs HOVÁTH, 016

29 Balázs HOVÁTH, 016

30 6 10 e = ull n ǣ 16 nn - n n od µ- Balázs HOVÁTH, 016

31

32 Scoe INTO ull on tuning egs gliss vi 1 gowl (thoat) thow away lectu! ite gliss vi ast od edal C B E sueall (u) lv od sueall (u) I "" sound oad ess ily gliss 11 uzz M hit (ute) ull Balázs HOVÁTH, 016 ess ily A ull 9 inst voice G ess ily E

33 1 II 9 1 vi gliss vi gowl (thoat) ite sueall (u) sound oad D gliss sueall (u) lv inst 0 voice vi M Balázs HOVÁTH, 016

34 Scoe 0 III : E tuning key C A "" lectu slow B ess ily lectu 9 IV E a teo : ess ily lectu od senza sinc senza sinc C B A G V G sueall (u) ess ily vi eeat eely then inish at Coda dolce lv CODA Balázs HOVÁTH, 016 od od glissando glissando lv ca -6 sec si (-x) lv Ócsa, 016 únius-úlius

Henrik Denerin. seals II. for cello and soprano. full score

Henrik Denerin. seals II. for cello and soprano. full score Henik Denein seals II o and ull scoe Henik Denein seals II (2014-15) o and duation: 5 seconds Notation: GENERA (all instuments) Scoe witten at laying itch All instuments ae tansosed and thei ats ae identical

More information

ELOQUENTIA espacio para flauta y orquesta

ELOQUENTIA espacio para flauta y orquesta Violin I 1 Manuel Sosa ELOQENTIA esacio aa lauta y oquesta MusikaSilentis New Yok 2010 The imay uose o the ba-lines is to seve as a device o synchonization. Ba-lines do not indicate accentuation o the

More information

This is This is This is (for David Foster Wallace)

This is This is This is (for David Foster Wallace) This is This is This is (fo David Foste Wallace) fo two alto saxophones in unison and pepaed piano Eic Wubbels (200910) Compose's Note Wite David Wallace committed suicide in late 200 In addition to the

More information

High Voice Two Violins Viola & Accordion

High Voice Two Violins Viola & Accordion CHISTOHE WILLIAM IECE ON A OEM O ADELAIE e t'adoe à l'égal de la voûte noctune om Les leus du Mal High Two Violins Viola Accodion 00 Chistohe William iece ASCA, All ights eseved o Katy e t'adoe à l'égal

More information

CHAPTER 5: Circular Motion; Gravitation

CHAPTER 5: Circular Motion; Gravitation CHAPER 5: Cicula Motion; Gavitation Solution Guide to WebAssign Pobles 5.1 [1] (a) Find the centipetal acceleation fo Eq. 5-1.. a R v ( 1.5 s) 1.10 1.4 s (b) he net hoizontal foce is causing the centipetal

More information

Preview Only. Legal Use Requires Purchase. Thomas Fats WAller Arranged by Eric Richards. Conductor 2nd E% Alto Saxophone

Preview Only. Legal Use Requires Purchase. Thomas Fats WAller Arranged by Eric Richards. Conductor 2nd E% Alto Saxophone The Jitterug Waltz Thomas ats WAller Arranged y Eric Richards instrumentation Conductor 1st E% Alto Saxohone 2nd E% Alto Saxohone 1st B% Tenor Saxohone 2nd B% Tenor Saxohone E% Baritone Saxohone 1st B%

More information

on the deconstruction of a cycle for 2 pianists and 2 percussion players Alberto C. Bernal

on the deconstruction of a cycle for 2 pianists and 2 percussion players Alberto C. Bernal on the deconstruction o a cycle or 2 ianists and 2 ercussion layers Alberto C. Bernal PERFORMANCE NOTES General: The dynamic indications between hooks reer to the intention dynamic, that can be dierent

More information

Lecture 23: Central Force Motion

Lecture 23: Central Force Motion Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces

More information

Niraj Sir. circular motion;; SOLUTIONS TO CONCEPTS CHAPTER 7

Niraj Sir. circular motion;; SOLUTIONS TO CONCEPTS CHAPTER 7 SOLUIONS O CONCEPS CHAPE 7 cicula otion;;. Distance between Eath & Moon.85 0 5 k.85 0 8 7. days 4 600 (7.) sec.6 0 6 sec.4.85 0 v 6.6 0 8 05.4/sec v (05.4) a 0.007/sec.7 0 /sec 8.85 0. Diaete of eath 800k

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding

More information

Chapter 5: Uniform Circular Motion

Chapter 5: Uniform Circular Motion Chapte 5: Unifom Cicula Motion Motion at constant speed in a cicle Centipetal acceleation Banked cuves Obital motion Weightlessness, atificial gavity Vetical cicula motion Centipetal Foce Acceleation towad

More information

Dream Theater. Paul Richards

Dream Theater. Paul Richards Commissioned y The niesity o loida Symhony Ochesta, Raymond Choaz, conducto, in celeation o thei 00 th anniesay season Deam Theate aul Richads Deam Theate aul Richads I Theshold II lace o Seeal Mysteies

More information

Eventually transatlantic signals! From Last Time. Electromagnetic Waves. The idea of electric fields. The electric field.

Eventually transatlantic signals! From Last Time. Electromagnetic Waves. The idea of electric fields. The electric field. Fom Last Time Electomagnetic waves Chages, cuent and foces: Coulomb s law. Acceleating chages poduce an electomagnetic wave The idea of the electic field. Today Electic fields, magnetic fields, and thei

More information

Sebastian Hilli. Paraphrase III. Soave dolore for Flute (+Alto Flute), Clarinet in Bb (+Bass Clarinet), Oboe (+English Horn), Horn and Bassoon

Sebastian Hilli. Paraphrase III. Soave dolore for Flute (+Alto Flute), Clarinet in Bb (+Bass Clarinet), Oboe (+English Horn), Horn and Bassoon 1 84 Sebastian Hilli Parahrase III Soave dolore or Flute (+Alto Flute), Clarinet in Bb (+Bass Clarinet), Oboe (+English Horn), Horn and Bassoon 2016 Coyright by the Comoser All Rights Reserved No art o

More information

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( ) : PHYS 55 (Pat, Topic ) Eample Solutions p. Review of Foce Eample ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? F G = F G + F G + F G = 4 +... = 3 z z Phs55 -: Foce Fields Review of Foce Eample

More information

Describing Circular motion

Describing Circular motion Unifom Cicula Motion Descibing Cicula motion In ode to undestand cicula motion, we fist need to discuss how to subtact vectos. The easiest way to explain subtacting vectos is to descibe it as adding a

More information

A Shrinking Emptiness/ Entropic Pleasures III

A Shrinking Emptiness/ Entropic Pleasures III Anders Hultqvist A Shrinking Etiness Entropic Pleasures III [Delineations (a), Version three] Commissioned y Ens MimitauLevande MusikKulturrådet 01 (Version 01, Version III 018) Anders Hultqvist A Shrinking

More information

INTRODUCTION. 2. Vectors in Physics 1

INTRODUCTION. 2. Vectors in Physics 1 INTRODUCTION Vectos ae used in physics to extend the study of motion fom one dimension to two dimensions Vectos ae indispensable when a physical quantity has a diection associated with it As an example,

More information

H5 Gas meter calibration

H5 Gas meter calibration H5 Gas mete calibation Calibation: detemination of the elation between the hysical aamete to be detemined and the signal of a measuement device. Duing the calibation ocess the measuement equiment is comaed

More information

STEVEN BRYANT. In This Broad Earth

STEVEN BRYANT. In This Broad Earth STEVEN BRYANT In This Broad Earth STEVEN BRYANT In This Broad Earth Written or and dedicated to Kevin Sedatole and the Michigan State University Wind Symhony lute I-II-III (doules Picc)* Ooe I-II Bassoon

More information

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009 Physics 111 Lectue 5 (Walke: 3.3-6) Vectos & Vecto Math Motion Vectos Sept. 11, 2009 Quiz Monday - Chap. 2 1 Resolving a vecto into x-component & y- component: Pola Coodinates Catesian Coodinates x y =

More information

Spring 2001 Physics 2048 Test 3 solutions

Spring 2001 Physics 2048 Test 3 solutions Sping 001 Physics 048 Test 3 solutions Poblem 1. (Shot Answe: 15 points) a. 1 b. 3 c. 4* d. 9 e. 8 f. 9 *emembe that since KE = ½ mv, KE must be positive Poblem (Estimation Poblem: 15 points) Use momentum-impulse

More information

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09 FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this

More information

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block?

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block? Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 13, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with

More information

Five Loons LLC No Erik Ferguson PERSPECTIVES OF A MAN SONG CYCLE FOR TENOR & FLUTE. Text by Stephen Crane. Complete Score.

Five Loons LLC No Erik Ferguson PERSPECTIVES OF A MAN SONG CYCLE FOR TENOR & FLUTE. Text by Stephen Crane. Complete Score. ive Loons LLC No. 102 Erik erguson ERSECTIVES O A MAN SONG CYCLE OR TENOR LUTE Text by Stehen Crane Comlete Score Comosed 2016 Erik erguson ERSECTIVES O A MAN SONG CYCLE OR TENOR LUTE Comosed 2015-2016

More information

PHYS 172: Modern Mechanics. Summer Lecture 4 The Momentum Principle & Predicting Motion Read

PHYS 172: Modern Mechanics. Summer Lecture 4 The Momentum Principle & Predicting Motion Read PHYS 172: Moden Mechanics Summe 2010 Δp sys = F net Δt ΔE = W + Q sys su su ΔL sys = τ net Δt Lectue 4 The Momentum Pinciple & Pedicting Motion Read 2.6-2.9 READING QUESTION #1 Reading Question Which of

More information

Physics 111 Lecture 5 Circular Motion

Physics 111 Lecture 5 Circular Motion Physics 111 Lectue 5 Cicula Motion D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Multiple Objects q A block of mass m1 on a ough, hoizontal suface is connected to a ball of mass m by a lightweight

More information

Your Comments. Conductors and Insulators with Gauss's law please...so basically everything!

Your Comments. Conductors and Insulators with Gauss's law please...so basically everything! You Comments I feel like I watch a pe-lectue, and agee with eveything said, but feel like it doesn't click until lectue. Conductos and Insulatos with Gauss's law please...so basically eveything! I don't

More information

Class 6 - Circular Motion and Gravitation

Class 6 - Circular Motion and Gravitation Class 6 - Cicula Motion and Gavitation pdf vesion [http://www.ic.sunysb.edu/class/phy141d/phy131pdfs/phy131class6.pdf] Fequency and peiod Fequency (evolutions pe second) [ o ] Peiod (tie fo one evolution)

More information

1121 T Question 1

1121 T Question 1 1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed

More information

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Physics 4A Chapter 8: Dynamics II Motion in a Plane Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.

More information

PROJECTILE MOTION. At any given point in the motion, the velocity vector is always a tangent to the path.

PROJECTILE MOTION. At any given point in the motion, the velocity vector is always a tangent to the path. PROJECTILE MOTION A pojectile is any object that has been thown though the ai. A foce must necessaily set the object in motion initially but, while it is moing though the ai, no foce othe than gaity acts

More information

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

Recitation PHYS 131. must be one-half of T 2

Recitation PHYS 131. must be one-half of T 2 Reitation PHYS 131 Ch. 5: FOC 1, 3, 7, 10, 15. Pobles 4, 17, 3, 5, 36, 47 & 59. Ch 5: FOC Questions 1, 3, 7, 10 & 15. 1. () The eloity of a has a onstant agnitude (speed) and dietion. Sine its eloity is

More information

( ) 4. Jones Matrix Method 4.1 Jones Matrix Formulation A retardation plate with azimuth angle y. V û ë y û. év ù év ù év. ë y û.

( ) 4. Jones Matrix Method 4.1 Jones Matrix Formulation A retardation plate with azimuth angle y. V û ë y û. év ù év ù év. ë y û. 4. Jons Mati Mthod 4. Jons Mati Foulation A tadation plat with aziuth angl Yh; 4- Linal polaizd input light é = ë û Dcoposd into th slow and ast noal ods és é cos sin é = sin cos ë- û ë û R ( ), otation

More information

Numerical Integration

Numerical Integration MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.

More information

Online-routing on the butterfly network: probabilistic analysis

Online-routing on the butterfly network: probabilistic analysis Online-outing on the buttefly netwok: obabilistic analysis Andey Gubichev 19.09.008 Contents 1 Intoduction: definitions 1 Aveage case behavio of the geedy algoithm 3.1 Bounds on congestion................................

More information

Olli Virtaperko Usvapatsas

Olli Virtaperko Usvapatsas Olli Virtaerko Usvaatsas or symhony orchestra ull score, transosed duration 1'0'' T e o s t o M u s i c i n l a n d Coyright by the Comoser No art o this ublication may be coied or reroduced in any orm

More information

Physics 121: Electricity & Magnetism Lecture 1

Physics 121: Electricity & Magnetism Lecture 1 Phsics 121: Electicit & Magnetism Lectue 1 Dale E. Ga Wenda Cao NJIT Phsics Depatment Intoduction to Clices 1. What ea ae ou?. Feshman. Sophomoe C. Junio D. Senio E. Othe Intoduction to Clices 2. How man

More information

8-3 Magnetic Materials

8-3 Magnetic Materials 11/28/24 section 8_3 Magnetic Mateials blank 1/2 8-3 Magnetic Mateials Reading Assignent: pp. 244-26 Recall in dielectics, electic dipoles wee ceated when and E-field was applied. Q: Theefoe, we defined

More information

Test 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.

Test 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction. Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae

More information

Physics 101 Lecture 6 Circular Motion

Physics 101 Lecture 6 Circular Motion Physics 101 Lectue 6 Cicula Motion Assist. Pof. D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Equilibium, Example 1 q What is the smallest value of the foce F such that the.0-kg block will not slide

More information

THE NAVIER-STOKES EQUATION: The Queen of Fluid Dynamics. A proof simple, but complete.

THE NAVIER-STOKES EQUATION: The Queen of Fluid Dynamics. A proof simple, but complete. THE NAIER-TOKE EQUATION: The Queen of Fluid Dnamics. A poof simple, but complete. Leonado Rubino leonubino@ahoo.it eptembe 010 Rev. 00 Fo www.via.og Abstact: in this pape ou will find a simple demonstation

More information

SOLUTIONS TO CONCEPTS CHAPTER 12

SOLUTIONS TO CONCEPTS CHAPTER 12 SOLUTONS TO CONCEPTS CHPTE. Given, 0c. t t 0, 5 c. T 6 sec. So, w sec T 6 t, t 0, 5 c. So, 5 0 sin (w 0 + ) 0 sin Sin / 6 [y sin wt] Equation of displaceent (0c) sin (ii) t t 4 second 8 0 sin 4 0 sin 6

More information

A car of mass m, traveling at constant speed, rides over the top of a circularly shaped hill as shown.

A car of mass m, traveling at constant speed, rides over the top of a circularly shaped hill as shown. A ca of mass m, taveling at constant speed, ides ove the top of a ciculaly shaped hill as shown. The magnitude of the nomal foce N of the oad on the ca is. A) Geate than the weight of the ca, N > mg. B)

More information

Physics NYB problem set 5 solution

Physics NYB problem set 5 solution Physics NY poblem set 5 solutions 1 Physics NY poblem set 5 solution Hello eveybody, this is ED. Hi ED! ED is useful fo dawing the ight hand ule when you don t know how to daw. When you have a coss poduct

More information

Tidal forces. m r. m 1 m 2. x r 2. r 1

Tidal forces. m r. m 1 m 2. x r 2. r 1 Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.

More information

Conflict Exam Issue. Sorry, Can t do it. Please see Kevin Pitts if you have any additional questions or concerns about this. Office is 231 Loomis

Conflict Exam Issue. Sorry, Can t do it. Please see Kevin Pitts if you have any additional questions or concerns about this. Office is 231 Loomis Conflict Exam Issue. Soy, Can t do it I was told that: Students can only be excused fom the scheduled final fo illness, death in the family o eligious holiday. No exceptions. Please see Kevin Pitts if

More information

Sparks. From Last Time. Other electric currents. Time-varying electric current. Eventually transatlantic signals! Electric Charge

Sparks. From Last Time. Other electric currents. Time-varying electric current. Eventually transatlantic signals! Electric Charge Electic Chage Fom Last Time Two types: plus and minus Foces between chages Like chages epel, opposite chages attact Coulomb s law: foce dops invesely w/ squae of distance Electic Cuent Flow of chages fom

More information

Relativity and Astrophysics Lecture 38 Terry Herter. Rain fall source to distance observer Distance source to rain fall frame

Relativity and Astrophysics Lecture 38 Terry Herter. Rain fall source to distance observer Distance source to rain fall frame Light and Tides Relativity and Astophysics Lectue 38 Tey Hete Outline etic in the Rain Fame Inside the hoizon One-way motion Rain Fall Light Cones Photon Exchange Rain all souce to distance obseve Distance

More information

Cecilia Damström. Op.27. Expressionen. Clarinet, Cello and Accordion 10'

Cecilia Damström. Op.27. Expressionen. Clarinet, Cello and Accordion 10' Cecilia Damström O7 Exressionen Clarinet, Cello and Accordion 10' 01 Exressionen O7 I Der Sechste Tag (Heinrich Camendonk) (clarinet, cello and accordion) II Einsamkeit (Alexe von Jalensky) (cello) IIIAquarelle

More information

Merging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)

Merging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.) Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms

More information

Preview Only. Legal Use Requires Purchase. Recorda me. JOE HENDERSON Arranged by KRIS BERG INSTRUMENTATION

Preview Only. Legal Use Requires Purchase. Recorda me. JOE HENDERSON Arranged by KRIS BERG INSTRUMENTATION Recorda me 1st E Alto Saxohone 2nd E Alto Saxohone 1st B Tenor Saxohone 2nd B Tenor Saxohone E Baritone Saxohone 1st B Trumet 2nd B Trumet rd B Trumet th B Trumet JOE HENDERSON Arranged y RIS BERG INSTRUMENTATION

More information

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below. Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

More information

PHYS 172: Modern Mechanics. Summer r p. Lecture 9 Motion Along a Curve Read Ch 5

PHYS 172: Modern Mechanics. Summer r p. Lecture 9 Motion Along a Curve Read Ch 5 PHYS 172: Moden Mechanics Summe 2010 Δ sys = F net Δt ΔE = W + Q sys su su ΔL sys = τ net Δt Lectue 9 Motion Along a Cuve Read Ch 5 Statics Static means that something doesn t change in time. What do

More information

Extra notes for circular motion: Circular motion : v keeps changing, maybe both speed and

Extra notes for circular motion: Circular motion : v keeps changing, maybe both speed and Exta notes fo cicula motion: Cicula motion : v keeps changing, maybe both speed and diection ae changing. At least v diection is changing. Hence a 0. Acceleation NEEDED to stay on cicula obit: a cp v /,

More information

Motion along curved path *

Motion along curved path * OpenStax-CNX module: m14091 1 Motion along cuved path * Sunil Kuma Singh This wok is poduced by OpenStax-CNX and licensed unde the Ceative Commons Attibution License 2.0 We all expeience motion along a

More information

Chap 5. Circular Motion: Gravitation

Chap 5. Circular Motion: Gravitation Chap 5. Cicula Motion: Gavitation Sec. 5.1 - Unifom Cicula Motion A body moves in unifom cicula motion, if the magnitude of the velocity vecto is constant and the diection changes at evey point and is

More information

CMSC 425: Lecture 5 More on Geometry and Geometric Programming

CMSC 425: Lecture 5 More on Geometry and Geometric Programming CMSC 425: Lectue 5 Moe on Geomety and Geometic Pogamming Moe Geometic Pogamming: In this lectue we continue the discussion of basic geometic ogamming fom the eious lectue. We will discuss coodinate systems

More information

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1 Physics 1501 Fall 2008 Mechanics, Themodynamics, Waves, Fluids Lectue 6: motion in two and thee dimensions III Slide 6-1 Recap: elative motion An object moves with velocity v elative to one fame of efeence.

More information

Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115;

Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115; WEEK-3 Recitation PHYS 3 eb 4, 09 Ch. 4: OC 9, 3,, 8. Pobles 0, 4, 38, 48, 77, 83 & 5; Ch. 4: OC Questions 9, 3,, 8. 9. (e) Newton s law of gavitation gives the answe diectl. ccoding to this law the weight

More information

Centripetal Force. Lecture 11. Chapter 8. Course website:

Centripetal Force. Lecture 11. Chapter 8. Course website: Lectue 11 Chapte 8 Centipetal Foce Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi PHYS.1410 Lectue 11 Danylov Depatment of Physics and Applied Physics Today we ae going to discuss:

More information

DESIGN OF BEAMS FOR MOMENTS

DESIGN OF BEAMS FOR MOMENTS CHAPTER Stuctual Steel Design RFD ethod Thid Edition DESIGN OF BEAS FOR OENTS A. J. Clak School of Engineeing Deatment of Civil and Envionmental Engineeing Pat II Stuctual Steel Design and Analysis 9 FA

More information

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

Physics 2A Chapter 10 - Moment of Inertia Fall 2018 Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.

More information

Momentum is conserved if no external force

Momentum is conserved if no external force Goals: Lectue 13 Chapte 9 v Employ consevation of momentum in 1 D & 2D v Examine foces ove time (aka Impulse) Chapte 10 v Undestand the elationship between motion and enegy Assignments: l HW5, due tomoow

More information

Quantum Fourier Transform

Quantum Fourier Transform Chapte 5 Quantum Fouie Tansfom Many poblems in physics and mathematics ae solved by tansfoming a poblem into some othe poblem with a known solution. Some notable examples ae Laplace tansfom, Legende tansfom,

More information

the silence that reigns... for large ensemble Heather Frasch A dissertation submitted in partial satisfaction of the requirements for the degree of

the silence that reigns... for large ensemble Heather Frasch A dissertation submitted in partial satisfaction of the requirements for the degree of the silence that eigns fo lage ensemble b Heathe Fasch A dissetation submitted in atial satisfaction of the equiements fo the degee of Docto of hilosoh in Music and the Designated Emhasis in Ne Media in

More information

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion Reading Assignment: Lab #9: The Kinematics & Dynamics of Cicula Motion & Rotational Motion Chapte 6 Section 4 Chapte 11 Section 1 though Section 5 Intoduction: When discussing motion, it is impotant to

More information

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website: Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula

More information

Music Diary. for soprano, flute, clarinet, violin, and percussion

Music Diary. for soprano, flute, clarinet, violin, and percussion Music Diary or sorano, lute, clarinet, violin, and ercussion LI Qi 201 Program Notes This is a iece or entertainment Have some un! :) Movements 1 Gossi!!! Girls always love gossi!!! Gossi always loves

More information

! " # $! % & '! , ) ( + - (. ) ( ) * + / 0 1 2 3 0 / 4 5 / 6 0 ; 8 7 < = 7 > 8 7 8 9 : Œ Š ž P P h ˆ Š ˆ Œ ˆ Š ˆ Ž Ž Ý Ü Ý Ü Ý Ž Ý ê ç è ± ¹ ¼ ¹ ä ± ¹ w ç ¹ è ¼ è Œ ¹ ± ¹ è ¹ è ä ç w ¹ ã ¼ ¹ ä ¹ ¼ ¹ ±

More information

Welcome to Physics 272

Welcome to Physics 272 Welcome to Physics 272 Lectue 1 Electic Chage and Coulombs Law Bob Mose mose@phys.hawaii.edu http://www.phys.hawaii.edu/~mose/physics272.html GO TO THIS SITE FOR ALL COURSE INFORMATION Phys-272 Bob Mose

More information

b) (5) What average force magnitude was applied by the students working together?

b) (5) What average force magnitude was applied by the students working together? Geneal Physics I Exam 3 - Chs. 7,8,9 - Momentum, Rotation, Equilibium Nov. 3, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults

More information

Sections and Chapter 10

Sections and Chapter 10 Cicula and Rotational Motion Sections 5.-5.5 and Chapte 10 Basic Definitions Unifom Cicula Motion Unifom cicula motion efes to the motion of a paticle in a cicula path at constant speed. The instantaneous

More information

Lecture 13 EXAM 2. Today s Topics: Rotational motion Moment of inertia. Tuesday March 8, :15 PM 9:45 PM

Lecture 13 EXAM 2. Today s Topics: Rotational motion Moment of inertia. Tuesday March 8, :15 PM 9:45 PM Lectue 13 Rotational motion Moment of inetia EXAM uesday Mach 8, 16 8:15 PM 9:45 PM oday s opics: Rotational Motion and Angula Displacement Angula Velocity and Acceleation Rotational Kinematics Angula

More information

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2.

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2. Chapte answes Heineann Physics 1 4e Section.1 Woked exaple: Ty youself.1.1 CALCULATING APPARENT WEIGHT A 79.0 kg student ides a lift down fo the top floo of an office block to the gound. Duing the jouney

More information

FARADAY'S LAW dt

FARADAY'S LAW dt FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,

More information

Lab #4: Newton s Second Law

Lab #4: Newton s Second Law Lab #4: Newton s Second Law Si Isaac Newton Reading Assignment: bon: Januay 4, 1643 Chapte 5 died: Mach 31, 1727 Chapte 9, Section 9-7 Intoduction: Potait of Isaac Newton by Si Godfey Knelle http://www.newton.cam.ac.uk/at/potait.html

More information

Today in Physics 218: radiation from moving charges

Today in Physics 218: radiation from moving charges Today in Physics 218: adiation fom moving chages Poblems with moving chages Motion, snapshots and lengths The Liénad-Wiechet potentials Fields fom moving chages Radio galaxy Cygnus A, obseved by Rick Peley

More information

Sea Fugue a song on an excerpt from a poem by Elee Kraljii Gardiner

Sea Fugue a song on an excerpt from a poem by Elee Kraljii Gardiner Sea Fugue a song on an excert rom a oem y Elee Kralii Gardiner or Mezzo sorano and Piano 2012 (ca 5:00) Christoher Gainey ( 1981) Dedicated to: Alison D'Amato and Lynne McMurtry With secial thanks to:

More information

Physics 211: Newton s Second Law

Physics 211: Newton s Second Law Physics 211: Newton s Second Law Reading Assignment: Chapte 5, Sections 5-9 Chapte 6, Section 2-3 Si Isaac Newton Bon: Januay 4, 1643 Died: Mach 31, 1727 Intoduction: Kinematics is the study of how objects

More information

Pietà. Violin, Cello and Piano For the Longleash Trio Duration: 18 Peter Kramer

Pietà. Violin, Cello and Piano For the Longleash Trio Duration: 18 Peter Kramer Pietà Violin, Cello and Piano For the Longleash Trio - - 01 Duration: 1 Peter Kramer PROGRAM NOTE Pietà was written during the Sring and Summer of 01 for Pala Garcia, ohn Poham and Renate Rohlng for the

More information

Relative motion (Translating axes)

Relative motion (Translating axes) Relative motion (Tanslating axes) Paticle to be studied This topic Moving obseve (Refeence) Fome study Obseve (no motion) bsolute motion Relative motion If motion of the efeence is known, absolute motion

More information

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed?

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed? Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 10, 2012 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with

More information

Stars for large orchestra.

Stars for large orchestra. Univesity o ouisville ThinkIR: The Univesity o ouisville's Institutional Reositoy Electonic Theses and Dissetations 5-2015 Stas o lage ochesta Matt Wetmoe 1989- Univesity o ouisville ollo this and additional

More information

alexander sigman struwl-2 for solo electric guitar (2012)

alexander sigman struwl-2 for solo electric guitar (2012) alexander sigman strwl- or solo electric guitar (0) strwl- (0) erormance notes general remarks A -sta notation is utilised throughout he to sta reers to let hand (ms) ingerings and articulations (see below)

More information

PHYSICS OF ASTROPHSYICS - Energy

PHYSICS OF ASTROPHSYICS - Energy PHYSICS OF ASTOPHSYICS - Enegy http://apod.nasa.gov/apod/ ENEGY esult of a foce acting though a distance. units = eg = dyne c i.e., foce x distance = g c /sec Two types: kinetic - enegy due to otion potential

More information

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session.

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session. - 5 - TEST 1R This is the epeat vesion of TEST 1, which was held duing Session. This epeat test should be attempted by those students who missed Test 1, o who wish to impove thei mak in Test 1. IF YOU

More information

Curvature singularity

Curvature singularity Cuvatue singulaity We wish to show that thee is a cuvatue singulaity at 0 of the Schwazschild solution. We cannot use eithe of the invaiantsr o R ab R ab since both the Ricci tenso and the Ricci scala

More information

Data Structures and Algorithm Analysis (CSC317) Randomized algorithms (part 2)

Data Structures and Algorithm Analysis (CSC317) Randomized algorithms (part 2) Data Stuctues and Algoithm Analysis (CSC317) Randomized algoithms (at 2) Hiing oblem - eview c Cost to inteview (low i ) Cost to fie/hie (exensive ) n Total numbe candidates m Total numbe hied c h O(c

More information

MMEA Central District - Jr. Jazz Audition Music. Quabbin Blues

MMEA Central District - Jr. Jazz Audition Music. Quabbin Blues r. azz Audition Music This iece has been commissioned by the or the exclusive use o district schools articiating in the 202 junior jazz auditions. Teachers o auditioning schools may rint and coy these

More information

Section 26 The Laws of Rotational Motion

Section 26 The Laws of Rotational Motion Physics 24A Class Notes Section 26 The Laws of otational Motion What do objects do and why do they do it? They otate and we have established the quantities needed to descibe this motion. We now need to

More information

Spectral colours. for Ensemble and tape. Javier Alejandro Garavaglia (1997)

Spectral colours. for Ensemble and tape. Javier Alejandro Garavaglia (1997) Sectal clus Ensemble and tae avie Aleand Gaavaglia (997) Ntes the emance The iece can be layed ith ithut the tae In the secnd case thee must be a ntice n the gam that claiies it ( examle: " Vesin ithut

More information

PY208 Matter & Interactions Final Exam S2005

PY208 Matter & Interactions Final Exam S2005 PY Matte & Inteactions Final Exam S2005 Name (pint) Please cicle you lectue section below: 003 (Ramakishnan 11:20 AM) 004 (Clake 1:30 PM) 005 (Chabay 2:35 PM) When you tun in the test, including the fomula

More information

30 The Electric Field Due to a Continuous Distribution of Charge on a Line

30 The Electric Field Due to a Continuous Distribution of Charge on a Line hapte 0 The Electic Field Due to a ontinuous Distibution of hage on a Line 0 The Electic Field Due to a ontinuous Distibution of hage on a Line Evey integal ust include a diffeential (such as d, dt, dq,

More information

Voltage ( = Electric Potential )

Voltage ( = Electric Potential ) V-1 of 10 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage

More information

Galilean Transformation vs E&M y. Historical Perspective. Chapter 2 Lecture 2 PHYS Special Relativity. Sep. 1, y K K O.

Galilean Transformation vs E&M y. Historical Perspective. Chapter 2 Lecture 2 PHYS Special Relativity. Sep. 1, y K K O. PHYS-2402 Chapte 2 Lectue 2 Special Relativity 1. Basic Ideas Sep. 1, 2016 Galilean Tansfomation vs E&M y K O z z y K In 1873, Maxwell fomulated Equations of Electomagnetism. v Maxwell s equations descibe

More information

Introduction to Systems of Differential Equations

Introduction to Systems of Differential Equations Chapte 4 Intoduction to Systes of Diffeential Equations Poject 4.1 Keple's aws and Planetay Obits The Section 4.1 poject in the text stats with Newton's invese-squae law of gavitation and outlines a deivation

More information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

More information

azim . =50 & \ \ .#! 4 .## O -ªªªªªªªªªªª Q. - F # % \ \ . F ( \ HANGING 1 METAL SHEET h 1 ..., -# j O... # j. #. glissando lentissimo

azim . =50 & \ \ .#! 4 .## O -ªªªªªªªªªªª Q. - F # % \ \ . F ( \ HANGING 1 METAL SHEET h 1 ..., -# j O... # j. #. glissando lentissimo =50 1 HORN as sounds) \ \ TROMBON \ \ \ \ PIANO A k ậ 7 O P molto legato 7 O Q O Q P j ## azim cuivré sound # 4 i - gliss # - k d gurgling sound 5 : breath + rapid fingers O -ªªªªªªªªªªª - d sp 6 h # O

More information