ABSTRACT. Music Theory & Composition Division School of Music. The initial concept of Unfading Echoes is to combine the elements of both

Σχετικά έγγραφα
Κάθε γνήσιο αντίγραφο φέρει υπογραφή του συγγραφέα. / Each genuine copy is signed by the author.

EE512: Error Control Coding

Homework 8 Model Solution Section

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

department listing department name αχχουντσ ϕανε βαλικτ δδσϕηασδδη σδηφγ ασκϕηλκ τεχηνιχαλ αλαν ϕουν διξ τεχηνιχαλ ϕοην µαριανι

Congruence Classes of Invertible Matrices of Order 3 over F 2

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

Areas and Lengths in Polar Coordinates

Αναερόβια Φυσική Κατάσταση

2 Composition. Invertible Mappings

derivation of the Laplacian from rectangular to spherical coordinates

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

Math 6 SL Probability Distributions Practice Test Mark Scheme

Section 1: Listening and responding. Presenter: Niki Farfara MGTAV VCE Seminar 7 August 2016

Srednicki Chapter 55

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Areas and Lengths in Polar Coordinates

Strain gauge and rosettes

Finite Field Problems: Solutions

MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)

The Simply Typed Lambda Calculus

Galatia SIL Keyboard Information

ST5224: Advanced Statistical Theory II

the total number of electrons passing through the lamp.

CRASH COURSE IN PRECALCULUS

Instruction Execution Times

[1] P Q. Fig. 3.1

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

Second Order Partial Differential Equations

þÿ¼ ½ ±Â : ÁÌ» Â Ä Å ÃÄ ²µ þÿä Å ÃÇ»¹º Í Á³ Å

C.S. 430 Assignment 6, Sample Solutions

Block Ciphers Modes. Ramki Thurimella

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

(1) Describe the process by which mercury atoms become excited in a fluorescent tube (3)

w o = R 1 p. (1) R = p =. = 1

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006

Statistical Inference I Locally most powerful tests

Approximation of distance between locations on earth given by latitude and longitude

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

ΠΡΟΓΡΑΜΜΑ ΜΕΤΑΠΤΥΧΙΑΚΩΝ ΣΠΟΥΔΩΝ ΔΟΥΚΑ ΒΙΟΛΕΤΤΑ - ΔΕΣΠΟΙΝΑ. Η Τέχνη της Πώλησης στη Φαρμακευτική Αγορά

Calculating the propagation delay of coaxial cable

Study of In-vehicle Sound Field Creation by Simultaneous Equation Method

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 24/3/2007

Matrices and Determinants

Georgiou, Styliani. Neapolis University. þÿ ±½µÀ¹ÃÄ ¼¹ µ À»¹Â Æ Å

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

What happens when two or more waves overlap in a certain region of space at the same time?

Concrete Mathematics Exercises from 30 September 2016

Dynamic types, Lambda calculus machines Section and Practice Problems Apr 21 22, 2016

PHOS π 0 analysis, for production, R AA, and Flow analysis, LHC11h

1 String with massive end-points

Section 8.3 Trigonometric Equations

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

Commutative Monoids in Intuitionistic Fuzzy Sets

Assalamu `alaikum wr. wb.

Second Order RLC Filters

Γιπλυμαηική Δπγαζία. «Ανθπυποκενηπικόρ ζσεδιαζμόρ γέθςπαρ πλοίος» Φοςζιάνηρ Αθανάζιορ. Δπιβλέπυν Καθηγηηήρ: Νηθφιανο Π. Βεληίθνο

Πρόβλημα 1: Αναζήτηση Ελάχιστης/Μέγιστης Τιμής

Solutions to Exercise Sheet 5

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

D Alembert s Solution to the Wave Equation

Dr. D. Dinev, Department of Structural Mechanics, UACEG

Επιβλέπουσα Καθηγήτρια: ΣΟΦΙΑ ΑΡΑΒΟΥ ΠΑΠΑΔΑΤΟΥ

Written Examination. Antennas and Propagation (AA ) April 26, 2017.

Other Test Constructions: Likelihood Ratio & Bayes Tests

Aluminum Electrolytic Capacitors (Large Can Type)

Partial Trace and Partial Transpose

Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1

4.6 Autoregressive Moving Average Model ARMA(1,1)

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Μορφοποίηση υπό όρους : Μορφή > Μορφοποίηση υπό όρους/γραμμές δεδομένων/μορφοποίηση μόο των κελιών που περιέχουν/

Tridiagonal matrices. Gérard MEURANT. October, 2008

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

ΑΡΙΣΤΟΤΕΛΕΙΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΘΕΣΣΑΛΟΝΙΚΗΣ ΤΜΗΜΑ ΟΔΟΝΤΙΑΤΡΙΚΗΣ ΕΡΓΑΣΤΗΡΙΟ ΟΔΟΝΤΙΚΗΣ ΚΑΙ ΑΝΩΤΕΡΑΣ ΠΡΟΣΘΕΤΙΚΗΣ

ΠΑΝΕΠΙΣΤΗΜΙΟ ΠΕΙΡΑΙΑ ΤΜΗΜΑ ΝΑΥΤΙΛΙΑΚΩΝ ΣΠΟΥΔΩΝ ΠΡΟΓΡΑΜΜΑ ΜΕΤΑΠΤΥΧΙΑΚΩΝ ΣΠΟΥΔΩΝ ΣΤΗΝ ΝΑΥΤΙΛΙΑ

Aluminum Electrolytic Capacitors

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

ΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ. «Προστασία ηλεκτροδίων γείωσης από τη διάβρωση»

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

Section 7.6 Double and Half Angle Formulas

Mean bond enthalpy Standard enthalpy of formation Bond N H N N N N H O O O


6.1. Dirac Equation. Hamiltonian. Dirac Eq.

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

Capacitors - Capacitance, Charge and Potential Difference

Durbin-Levinson recursive method

TMA4115 Matematikk 3

Every set of first-order formulas is equivalent to an independent set

VBA ΣΤΟ WORD. 1. Συχνά, όταν ήθελα να δώσω ένα φυλλάδιο εργασίας με ασκήσεις στους μαθητές έκανα το εξής: Version ΗΜΙΤΕΛΗΣ!!!!

Αναλυτική προσέγγιση στο έργο του Αθανάσιου Ζέρβα, RITUALS for Viola του Ανδρέα Γεωργοτά

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

On a four-dimensional hyperbolic manifold with finite volume

ΔΙΑΤΜΗΜΑΤΙΚΟ ΠΡΟΓΡΑΜΜΑ ΜΕΤΑΠΤΥΧΙΑΚΩΝ ΣΠΟΥΔΩΝ ΣΤΗ ΔΙΟΙΚΗΣΗ ΕΠΙΧΕΙΡΗΣΕΩΝ ΘΕΜΕΛΙΩΔΗΣ ΚΛΑΔΙΚΗ ΑΝΑΛΥΣΗ ΤΩΝ ΕΙΣΗΓΜΕΝΩΝ ΕΠΙΧΕΙΡΗΣΕΩΝ ΤΗΣ ΕΛΛΗΝΙΚΗΣ ΑΓΟΡΑΣ

Higher Derivative Gravity Theories

Transcript:

ABSTRACT Title of dissertation: UNFADING ECHOES Chao-Jung Wu, Doctor of Musical Arts, 2011 Dissertation directed by: Professor Thomas DeLio Music Theory & Composition Division School of Music The initial concept of Unfading Echoes is to combine the elements of both Western and Eastern music in a profound way; the violin and the Chinese fiddle erhu, are used to symbolize the two cultures. The erhu a Chinese traditional instrument is normally tuned to D4 and A4, which is the same as the two middle strings of the violin. Comparing its timbre with the violin s, the erhu emphasizes higher overtones; its fundamental is weaker than some of the partials, which gives its sound a nasal quality. The traditional Chinese piece for the erhu, The Moon Reflected in Er-quan, which is often considered one of the most important masterpieces in China, inspired this work in various respects. In small scale, its pitches, melodic contour, and its rhythms are thoroughly utilized in Unfading Echoes; in larger scale, the ways of varying theme, the slow pace, the ambiguous edges between sections/phrases have also considerably influenced the design of this piece. The piece can be divided into three major sections (see table 1 & figure 1). Proportionally, the sum of section I and II is roughly equal to section III; the overall plan also suggests that the contour design reflects quasi-symmetry.

m.# Duration (seconds) I(i) 0 00 ~1 00 1-9 0 Note Detuned violin solo I I(ii)-1 1 00 ~2 00 10-22 0 Tape enters I(ii)-2 2 00 ~4 00 2-4 120 I(ii)- 4 00 ~7 00 44-80 180 II II 7 00 ~10 00 81-114 180 III III(i) 10 00 ~11 0 115-12 90 Only tape III(ii)-1 11 0 ~1 17 127-147 107 Violin cadenza III(ii)-2 1 17 ~14 52 148-15 95 Tape re-enters III(ii)- 14 52 ~15 9 1-174 47 III(ii)-4 15 9 ~1 51 175-187 72 III(iii)-1 1 51 ~19 5 188-217 14 III(iii)-2 19 5 ~20 14 218-22 9 III(iii)- 20 14 ~20 227-20 22 Table 1 table of Unfading Echoes. Figure 1 Overall plan (dark violin, light tape)

The timbral evolution, mainly established by the tape, includes two phases. From the beginning to 11 0 is a progress of tape splitting from the violin as its extension and eventually draws emphasis on the attack sound, which finally accumulates to white noises. The second phase starts after the violinist s cadenza at 1 17, where the tape shifts its function from a violin s follower or competitor to a main character. Finally, the two detuned strings at the beginning are designed to relate to the open strings of the erhu. The unusual tuning gives listeners a clue which remains unsolved until its reoccurrence at the end when the intro phrase of The Moon Reflected in Er-quan becomes the closing phrase of the whole piece. The idea corresponds to the sense of infinity in Chinese esthetics endless cycles.

UNFADING ECHOES for violin and tape by Chao-Jung Wu Dissertation submitted to the Faculty of the Graduate School of the University of Maryland, College Park in partial fulfillment of the requirements for the degree of Doctor of Musical Arts 2011 Doctoral Committee: Professor Thomas DeLio, Chair Associate Professor James Fry Professor Denny Gulick Associate Professor Mark E. Wilson Dr. Daniel Zimmerman

Unfading Echoes is dedicated to my parents, my brother, my husband, and Chun-Hsin Jenny Wu.

Notes Violin Two violins are required; one normal tuned and another detuned as: The piece starts with detuned violin; the violinist should change to specified violin when indicated. If desired, the soloist may perform m.127~147 with tempo ad lib.; use Version [B] with separated sound-files. * In m.1~20, play on open strings as much as possible. * In m.10~20, finger the notes as if playing with normal-tuned violin. Tape Version [A]: one stereo sound file, total length: ca. 20 Version [B]: two stereo sound files: a sound engineer or a pedal (if tape is controlled by violinist) is needed to trigger the second clip. Clip 1 (0 00 ~10 00 ): starts initially with violinist. Clip 2 (1 12 ~end): starts at m.127 with violinist s cue. Notation (square notehead) use left hand tap on ricochet fingerboard aprrox. pitch accel. highest pitch on indicated string wide vibrato (if specified, vibrate with indicated pitch) behind bridge (on string specified) or pitch ad lib short gliss up/down after reach the pitch longer gliss up/down after reach the pitch snap pizzicato (Bartók pizzicato)

Violin q 0 Con sord. j L 4 7 niente F π π 4 Senza sord. 5 π fl π π θ 7 fl θ π, Θ 1'00" 1'07" 10 αe Θ α e ú Ï niente e ( ( θ niente Tape 1'02" 1'05" 1'08" * Tuning: 1

1'14" 1'18" 1'22" 1'2" 12 e A 1'1" (echo) 1'14" 1'18" niente θ, niente e ord.... sul ponticello ú ( 1'2" niente + 4 4 4 4 1'0" 1'5" 1'40" 1 4 ord. Con sord. ord.... sul tasto π ord. e 4 4 4 1'1", 2 1'8" α α Θ

1'45" 1'49" 1'5" 1'57" 19, π Senza sord. niente 2 niente N N 1'47" θ θ 1'52" α φ 2 2 2 1'58" α 2'00" 2'04" 2'09" 2'14" 2 N N * Change to normal tuned violin 4 4 4 4 2'05" α (echo) n n, arco n n n n n n n n n n n n n 2'10" α,, µ 2'17"

2'21" 2'28" 2'4" 27 arco Μ,, sub. 5 5 ord. sub. 5 2'22" l l Θ l l (metalic) 5 5 Θ 2'5" 2'8" µ 2'40" 2'4" 0 arco 2'4" 4 φ 7 α µ 2'47" @ (gliss down) α 4 4 4 4

2'52" 2'57" '01" 2 4 α 5 (let ring) 4 4 4 }}}}}}}}}}}}} (gliss down) α α 2'58" α 5 5 5 b µ α '05" α α φ '07" '1" '19" 5 arco µ α sub. µ µ! 5 '21"!

'25" '1" 8 '27" α µ µ α '7" Θ 4 4 4 '5" 5!!!!!! fl 4 '8" '4" '50" '5" 40 4 4 4 4 2'40" ã ã ã ã ã fl α α α '4" φ '4" α α ) (sharp pizzicatos) 5 5 5 5 Ν Ν Ν Ν Ν φ 4 4 4 4

4'00" 4'05" 4'09" 44 4 arco α µ sub. sul ponticello ord. µ 4 α µ π 4 4 4 4'04" 4 4 4 4'14" 4'21" 4'25" 47 4'18"!,, }}}}}}, Θ α ::::: : : : : : : : π (noises) (gliss down) 7 : : : : 4'28"

4'29" 50 α 4 4'" µ. α 4'0" α 4 4 4 : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 4'8" 4'42" 52 arco α α : : : : ; ; ; ;: : : µ α µ : ; ;; ; ; ;; ; ;: : : : 4 4 arco, ; ; ;; ; ;: : : : α α ; ; ;; ; ; ; (noises) ;; ; ;; ; ; ; ; ; : : : : : 4 4! fl 8

4'47" 4'52" 4'5" 54,, arco α α α µ µ 5 4'48" 4'50" α 4'49" µ α µ!! π α! 4'59" θ!!! α 5 5 5 5'0" 5'09" 57 5 arco, α µ 4 5 5 5 θ!! : : : : :: : : : ::::: α 4 4 4 9

5'1" 5'21" 59 4 α 5, µ α α α arco π 4 5 4 4 }}}} ) (gliss up to C) 5 5 α α φ αα φ :::: 5'27" 5'1" 5'5" 1,, α, α µ 5 α α θ π α arco α µ : : : : : : : : : : ;;; ; ::: : ::; ; ;;;;;:: σ 10 ö ö ö µ ö ö (self-gliss pitch) 5'8"

5'9" 5'4" 5'47" 4 α µ ν ν ν 4 σ π α α α? 4 4 4 5'51" 5'5" '00" 7 4 4 4 σ 4 µ α α arco α α!, sub. π µ,, 5 :4 µ, 4 4 4 4 Θ α 11

'05" '10" '14" '18" '22" 70 α α sub. α ( α α µ µ arco Ν 4 '07" ö ö ö µ '24" α 4 4 4 '2" '1" '7" 75 4 4 4 4 Ν Ν φ α α 5 5 5 5 ν α Ν 5'" ), α 12 µ Ν sub. µ µ )

'4" '49" '55" 78 ( Θ Con sord. Θ '44" 7 arco Θ 4 4 4 4 ord. Ν Ν π 5 fl '57" 5 5 5 5 7'00" 7'0" 7'12" 7'17" 81 5 Senza sord. Ν niente α α Ν, sub. 4 α, ord.... press hard... ord., 5 5 5 }}}}} 7'04" α α 7'10" α µ }}}}}}}}}}}}}}}}}} 1 4 4 4 α 7'1" 7'14" }}}}}}}} ( gliss up)

7'22" 7'2" 7'1" 7'" 85 α }}}}}}}}}}}}}}}} 7'25" αçç 4 4 4 4 α ( Ν Ν Ν Ν π Ν 7'29" ç ç Ν 5 5 }}}}}}}}}}}}}}}}}}}}}}}}}}}} ç 5 (gliss up) 7'8" α 7'41" α α µ 7'42" 7'48" 7'55" 89 7,,,,,,, arco Θ µ Ν 7'45" ) α α µ 7'50" α (gliss up) }}}}}}}}}}}}} 14

8'02" 8'09" 8'1" 8'19" 92 Ν Ν α Ν Ν Ν µ 8'07" ç ç fl sub. 8'11" ç 5 5 5 5 α 8'14" ç ord.... press hard... ord. }}}}}}} 8'2" 8'27" 8'1" 8'" 9 φ φ, }}}}}}}}}}}}}}}}}}}}}}}}}} α α µ 5 Ν Ν Θ φ φ 8'0" 5 4 4 4 4 arco Ν Ν 8'" non Vibrato 5 5 5 5 15

8'41" 8'47" 8'5" 100 5 ν Ν µ Ν Ν Ν Ν 4 Ν 5 5 5 5 π 8'48" φ z z z z z z z z z zzz z z zz z 4 4 4 8'57" C 5 5 5 8'58" 9'04" 9'10" 10 5 5 5 5 C C C ν ν pitch ad lib. θ sub. µ ν θ ( sub. 9'12" ) µ 1

9'14" 9'18" 9'2" 10 9'1" π 4 4 4 4 Ν Ν Ν Ν Ν µ µ Ν Ν α α Ν Ν,,,,, 9'27" CC 5 5 5 5 9'27" 9'" 109 5 5 5 5 Ν C C C C CC C C C C CC CC C C Ν µ Ν µν Ν 9'2" 4 4 4 4 5 ) φ θ µ µ µ 17

9'8" 111 sub. θ µ µ 9'44" 9'41" 5 ) ) ) ) ) µ µ 5 5 5 5 9'45" 9'51" 9'5" 112 5 α [ ( 5 9'49" α α 5 }}}}}}}}}}}} 4 4 4 Ν α α Ν µ µ Ν ν1 ord. Ν1ν Ν (let ring) 0/ 0/ 0/ 5 4 0/ 18

n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n 10'00" 10'10" 115 0/ 7 5 0/ 0/ a C α α α C 7 7 a C α CC CC C C C C C 5 5 0/ 7 5 5 5 5 D a α Θ a Θ a 4 LLLLLLLL Ï Ï 4 4 αa C CC θ C 2 a α a 2 α C b C n n n n n n n n n n n n n n n 5 5 5 10'18" 10'24" 10'29" 117 5 4 5 19

n n n n n n n n n n n n n n n 10'4" 10'40" 10'48" 120 5 7 01 7 5 5 5 n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n n 2 2 2 7 n n n n n n n n n n n n n n n n n n n n n n 7 7 ) fl 5 B E C C C D 01 01 01 ZLZ \ \ 7 7 7 \ \ 11'00" 11'08" 11'15" 11'22" 12 7 7 5 7 7 7 ZZZ HH (white noise) H Θ a Θ a W NN OO MHHHH 7 (white noise) 7 [ XÏ 7 ú Ï Ï ú ))))))))) 20 5 5 5

127 (11'0") q β 0 tempo ad lib. (* square notehead: left hand tap on fingerboard) ric....ord. gradually press hard 5 4 2 θ θ fl π flπ 10 ord. 5 5,,, θ,, + ord. sul ponticello Θ! Θ µ sub. gradually press hard press hard ponti. 12 5 µ µ :2 5 Θ, θ 7 θ :4 θ,,, sub. α µ! sub. λλλλλλλλλ ric....ord. 14 ord. α wide vibrato 4 5,,,,,,, ric....ord. ord., sub. 5 17 5 4 + θ Θ µ? µ Θ! fl sub. π flsub. sul tasto 140 ric....ord. (quick gliss down) θ α 5 ¹ ¹ e e e e fl π e ¹ ¹ e ¹ e¹ ¹ ¹ ¹ e e e e e e e ν approx. pitch ¹ 5 9 θ :8 θ 21

142 5 ν?,, 14 + µ,,,, -,, + 5 ric....ord. ric....ord. α ric....ord. θ α ric....ord. 145 4 θ α µ! ¾ ¾ ¾µ µ µ + Τ ric....ord. 7 5! Cue Clip 2 Ver. [A] 1'12" Ver. [B] 0'00" 147 4 a tempo α fl sub. 1'17" 0'05" 2 1'24" 0'12", µ, 4 1'27" 0'15" press hard... ord. ¾ 5 4 4 4 1'12" 0'00" φ 1'18" 0'0" 1'19" 0'07" 1'21" 0'09" α 22 2 2 2 1'25" 0'1" 4 4 4 5 5 5

151 5 5 5 1'2" 0'20" α 1'5" 0'2" α,,, ν 1'8" 0'2" sub. α 1'40" 0'28" α α 1'42" 0'0" α niente 5 (metalic)!!!!! 154 1'4" 0'4" 1'47" 0'5" 1'5" 0'41" 4 α 4 4 4 µ α µ CAA AAA AA A 2 A A A A A A A α A AA A

15 α α ric....ord. µ 14'01" 0'49"? sul ponticello θ? 7 7 7 7 14'05" 0'5" ord. Ÿ}}}}}}}}}}}}}}}}}}}}}} Μ fl 14'0" 0'54" θ µ 14'08" 0'5", 5 5 5 5 14'1" 1'01" 14'19" 1'07" 14'2" 1'14" 158 5 sul tasto ord. trem. ord.... sul ponticello π 5 5 5??? α 24

11 14'0" 1'18" θ α α 2 2 2 2 14'4" 1'22" 14'5" 1'2" α 5 5 5 5 5 14'7" 1'25" arco ord. wide vibrato λλλλλλ Θ, π α 14'41" 1'29" α µ 14'4" 1'1" 14'47" 1'5" 14'52" 1'40" 14 4 4 4,????????? 14'50"???? 1'8" (birds-like) (behind bridge) sul A X???????? α Θ 4 25

17 14'57" 1'45" arco α 5 15'02" 1'50" sub. θ µ 4 5 5 5 15'07" 1'55"?? 4 4 4 19 4 15'08" 1'5" arco 15'1" 2'01" 5 15'17" 2'05" α θ α sub. 4 4 4 α 5 5 5 2

15'2" 2'11" 15'0" 2'18" 172 α, µ α niente α µ α 4 α 15'25" 2'1" CC αc CC 15'29" 2'17" α α α 4 4 4 174 4 15'4" 2'22", λλλλλλλλλ wide vibrato 15'9" 2'27" µ gradually wide vibrato 5 15'4" 2'1" ord., µ niente 4 4 4 15'5" 2'2" µ 27 15'42" 2'0" 5 5 5 15'4" 2'4" α? 15'47" 2'5"

15'49" 2'7" 15'55" 2'4" 177 tremolo crooked bow l.h. ord. ¾ α arco ord. µ 4 15'5" 2'1" α 5 α 15'57" 2'45" C C C C C 4 C C C C CCC C C C C C CC C C CCCCCCCCC C C C CC CC CC 4 4 1'02" 2'50" 1'07" 2'55" 1'1" '01" 179 4 Θ ¾ 5 ord. - 4 4 α 5 5 α 4! fl 5 28

1'20" '08" 1'24" '12" 1'1" '19" 1'" '24" 182 4,,, α 4 θϑ α ACC 4 4 4 CA 1'5" '2" 4 4 4 1'40" '28" 1'45" '" 1'51" '9" 18 4 4 4 4 5,,, sub. 5 5 5 Ÿ Η }}}}}}}}}}}}}}}}} 5 1'50" '8" α λλλλ 4 4 4 4? (gliss up) µ 29

189 1'5" '44" 17'01" '49" ord.... sul ponticello ord.... sul ponticello Θ fl 17'0" '54" ord., α, µ 17'09" '57" 17'11" '59" 192, α,, 17'1" 4'04" Ÿ}}}}}}}}}}} approx. pitch eee 17'21" 4'09" α µ ( α gliss tr. between Eb Ÿ}}}}}}}}}}}}}}}}}} sub. π α,,,,,,,,,,,,,,, 17'19" 4'07" 0

195 17'2" 4'14" λλλλλλ wide vibrato (Ab) α fl 17'1" 4'19" niente 17'29" 4'17" 197 17'" 4'24" µ, sul A 17'41" 4'29" Θ 5 17'4" 4'4" α, 4 D Τ fl Θ 17'44" 4'2" 7 1 5 5 5 Ÿ 4 4 4

17'52" 4'40" 200 4 sub., 17'57" 4'45" 5 ½ ½ ½ ord.... sul ponticello 4 4 4 5 5 5 202 18'0" 4'51" µ Ricochet α α ord. 4 4 4 4 18'09" 4'57" flsub. α α α 2 2 2 2 18'14" 5'02" Θ, ¾ ¾ ¾ ¾ ¾ 5 5 5 5 2

18'17" 5'05" λλλλλλλλλλλλλλλλλλλλλλλλλλλλλλλλλ wide vibrato 205 5 π 18'2" 5'11" cresc. 18'29" 5'17" 18'5" 5'2" ( (let ring) L j 4 5 5 5 λλλλλ 18'2" 5'20" α µ 5 α! 4 4 4 18'42" 5'0" 18'47" 5'5" 209 L j 4 4 4 4 * Change to detuned violin. 5 A 5 5 5 18'50" 5'8" 5 7 7

211 18'5" 5'41" π ( ( ( 4 19'00" 5'48" arco, sub. 5 19'05" 5'5" µ C CC π 4 4 4 19'02" 5'50" α C α C 5 5 5 214 19'11" 5'59" 19'15" '0" ( 4 19'19" '07" ( 19'24" '12" fl sub.???????? 4 4 4 4

19'28" '1" 19'5" '2" 19'40" '28" 218 sul tasto... ponticello ord. sub. 4 4 4 4 5 α ric....ord. α µ α µ α 221 19'44" '2" Ÿ}}}}}}}}}}}}}}}}}}}} ord. 19'48" '" Ÿ Ÿ Ÿ α½ ½ ( ½ (gliss up after trill) Ÿ ½ Ÿ ½ Ÿ ½ Ÿ ½ ½ ½ ½ ½ ½ ½ 19'52" '40" 5 5 5 (h) (highest pitch) (let ring) Ricochet ord. (Roll from string Iand II to III and IV.) 4 4 4 # 5 # 19'57" '45" ) ) 4 5

224 4 4 4 19'58" '4" ric....ord. π λλλλλλ wide vibrato III IV 5 5 5 20'0" '51" () 4 4 4 20'09" '57",,,,, 5,,,,,,, ν ν ν ν pitch ad lib. 7 II III on bridge. slow bow. II III II III fl sub. 4 ) ) ) 5 4 227 20'14" 7'02" (on bridge. slow bow...) 20'19" 7'07" 20'24" 7'12" sub. 20''29" 7'17" gradually ord.... (let ring) 20'17" 7'05" 20'2" 7'04" Τ