You have met function of a single variable f(x), and calculated the properties of these curves such as

Size: px
Start display at page:

Download "You have met function of a single variable f(x), and calculated the properties of these curves such as"

Transcription

1 Chaper 5 Parial Derivaive You have me funcion of a ingle variable f(, and calculaed he properie of hee curve uch a df d. Here we have a fir look a hee idea applied o a funcion of wo variable f(,. Graphicall hi i ea o repreen a he variaion of he heigh of a urface above a plane a a poin wih coordinae (,. 5.1 Fir Parial derivaive The lope of he funcion f(, in general will depend on he direcion in which i i calculaed. We will ar here b calculaing he lope in he and direcion. To ake he parial derivaive wih repec o we mu keep fied and var b a mall amoun, δ. Thi i denoed b = lim δ 0 f( + δ, f(,. (5.1 δ Similarl he parial derivaive wih repec o i calculaed b keeping fied and varing = lim δ 0 f(, + δ f(,. (5.2 δ Thee definiion are much he ame a ordinar derivaive obained b varing one variable and keeping all oher conan. For eample conider he funcion We can define higher derivaive in he ame wa f(, = (5.3 = (5.4 = (5.5 = 2 f 2 (5.6 = 2 f 2 (5.7 = 2 f = 2 f 48 (5.8 (5.9

2 CHAPTER 5. PARTIAL DERIVATIVES 49 Noe ha provided he parial derivaive are coninuou a he poin in queion hen = 2 f i.e. he order in which we ake he derivaive doe no affec he reul. In our earlier eample 5.2 Talor Theorem (5.10 = 2 (5.11 = 2. (5.12 You have me he idea of a erie epanion for a funcion of a ingle variable. If we epand f( abou he poin 0 he reul i a Talor erie f( f( 0 + f ( 0 ( 0 + f ( ( = f (n ( 0 ( 0 n. (5.14 n! n=0 We can performa imilar epanion for a funcion of wo variable abou he poin ( 0, 0 f(, = f( 0, [ 2 ] f 2! 2 ( f + 2 f 2 ( (5.15 where = ( 0 and = ( 0. Thi epreion can be epreed more uccincl in he noaion of vecor calculu a ou will ee ne ear. 5.3 Toal differenial f(, = f( 0, 0 + ( n f (5.16 If we allow a mall change in boh and hen we can obain he oal change in he funcion f(, denoe b df a follow n=1 df = f( + δ, + δ f(, (5.17 = d + d (5.18 where we have negleced he higher order erm (δ 2 ec. in he approimaion. Thi epreion i known a he oal differenial of f. For eample conider he funcion f(, = in df = din + dco (5.19 Now uppoe ha = ( i.e. i a funcion of. The oal derivaive of f wih repec o i hen df d = + d d (5.20

3 CHAPTER 5. PARTIAL DERIVATIVES 50 Anoher wa o ee hi i a follow. If we make a mall change in f(,, where = ( hen we have: ( f( + δ, ( + δ f + δ, ( + d d δ + O(δ2 Eac oal differenial f(, ( + df d = + d d ( + d d δ + O(δ 2 The eample in he la ecion i known a an eac differenial, becaue if we ar from din + dco hen we can find he funcion f(, = in ha will produce hi differenial. Anoher eample i he differenial d + d, which mu reul from a funcion f(, = + K. Some differenial are no eac, for eample d + d. (5.21 Here he fir par inegrae o 1 2 2, bu he econd par inegrae o In general if we have a differenial hen o for i o be eac, we require 5.4 Reciproci and cclic relaion A(, d + B(, d (5.22 = A (5.23 = B (5.24 A = B. (5.25 Suppoe we have a relaion beween hree variable z = z(,. The oal differenial of hi epreion i ( ( dz = d + d. (5.26 Bu we could alo wrie = (, z d = ( d + z If we ubiue hi epreion ino our fir reul for dz we obain ( ( [( ( dz = d + d + z ( ( ( ( dz = d + d + z ( dz. (5.27 dz ] ( (5.28 dz (5.29

4 CHAPTER 5. PARTIAL DERIVATIVES 51 If we e d = 0 hen we obain which i he reciproci relaion. ( ( = 1/ Alernaivel if we e dz = 0 hen we obain ( 1 = Thi i he cclic relaion. ( z ( (5.30 ( Chain Rule Suppoe ha boh = ( and = (, i.e. boh and depend on a parameer. If we have a funcion f(, hen we can calculae i derivaive wih repec o b uing he chain rule df d = d d + d d (5.32 Thi i known a he chain rule, and i paricularl ueful if we are calculaing he derivaive of f along a paricular pah ha i defined paramericall (i.e. in erm of. Anoher wa o ee hi i b uing alor heorem δf = f( + δ, + δ f(, δ + δ + (O(δ2, δ 2, δδ (5.33 If we ubiue δ = d d δ + O(δ2, and imilarl for δ hen we obain δf ( d d δ + ( d d δ + O(δ 2. (5.34 If we divide hrough b δ and ake he limi δ 0 hen we obain he chain rule reul. 5.6 Change of variable I i ofen convenien o change he variable ha we ue o epre a paricular funcion. Suppoe we have f(, bu wan o work in erm of new variable and, ha are relaed b = (, and = (,. The derivaive of f wih repec o our new variable can be epreed a follow ( ( ( ( ( = + (5.35 ( = ( + ( ( (. (5.36 We can how ha hi i rue b uing Talor heorem again. We can obain Eq. (5.35 a follow (neglecing erm O(δ 2 ec. hroughou. δf = f( + δ, + δ f(, (5.37 = f(( + δ,, ( + δ, f(, (5.38 f( + δ, + δ f(, (5.39 ( ( ( ( δ + δ (5.40

5 CHAPTER 5. PARTIAL DERIVATIVES 52 which produce Eq.(5.35 in he limi δ 0. For eample uppoe we wih o calculae ( ( and, bu have f(, where ha = and = +. We impl appl he reul aed above ( = 1 (5.41 ( = 1 (5.42 ( ( ( = + (5.43 ( = 1 (5.44 ( = 1 (5.45 ( ( ( = +. (5.46 Alernaivel, uppoe we have a funcion in Careian coordinae f(, bu wih o work in( polar coordinae, where = r coθ and = r in θ. In erm of hee new variable we can calculae r θ. ( ( ( ( ( = + (5.47 r θ r θ r θ ( ( = coθ + in θ (5.48 ( and imilarl for θ. r 5.7 Anali of aionar poin of a funcion of wo variable For a funcion of a ingle variable a aionar poin occur when df d naure of hi poin b eamining he econd derivaive d2 f d. 2 (a d2 f d 2 > 0 he lope i increaing o we have a minimum. (b d2 f d 2 < 0 he lope i decreaing o we have a maimum. (c d2 f d 2 = 0 poin of infleion. For a funcion of wo or more variable aionar poin ill occur when = 0. We can characerie he = 0 and = 0. (5.49 However, he naure of hee aionar poin i a lile more varied. We can have maima and minima a before, bu in addiion o hee we can alo have a addle poin, where we have a maimum

6 CHAPTER 5. PARTIAL DERIVATIVES 53 in one direcion and a minimum in anoher. If we anale he econd erm in he Talor erie we can pin down he naure of he aionar ( poin. We will do hi uing he mari mehod from earlier in he coure. If we wrie = hen [ 2 ] f 2 ( f + 2 f 2 ( 2 = T H (5.50 where H = ( 2 2 = ( f f f f (5.51 i he mari of econd derivaive known a he Heian mari, and we have inroduced a hor hand for he econd derivaive. Our funcion hould increae in all direcion from a minimum, o T H > 0. If hi i rue hen H hould alwa have poiive eigenvalue. Similarl if we are a a minimum hen H hould alwa have negaive eigenvalue. If we are a a addle poin hen we hould have one poiive and one negaive eigenvalue. Equivalenl (i Minima f 2 < f f and boh f, f > 0 (boh eigenvalue poiive. (i Maima f 2 < f f and boh f, f < 0 (boh eigenvalue negaive. (i Saddle f 2 > f f (eigenvalue of mied ign. If f = f = 0 or if he eigenvalue are equal o zero hen furher anali of he fied poin i necear o deermine i characer. 5.8 Thermodnamic Man phical quaniie can be epreed in erm of parial derivaive, for eample The coefficien of hermal epanion α = 1 V ( V T P Molar hea capaci a conan volume c p = T ( T The reciproci relaion and he cclic relaion are ueful for manipulaing derivaive like hee. Calculaing he ae of a em can be done b minimiing i free energ. To find he abili of he em he naure of he aionar poin mu be found. The inabili of a phae of maer can poin o inereing phical effec, uch a phae eparaion which ou will learn more abou laer in our coure. P. 5.9 Problem 1A. Show ha 2 f = 2 f for he following funcion (a f(, = (b f(, = in( (c f(, = e ln( +

7 CHAPTER 5. PARTIAL DERIVATIVES 54 (d f(, = A. Evaluae + when (a f = 1 + (b f = ln (c f = f( 3B. Find which of he following differenial form Pd + Qd are eac. If he are eac, find a funcion f uch ha df = Pd + Qd, and he general oluion of he equaion Pd + Qd = 0. (i d + d (ii d + 2 d (iii ( + d + ( d (iv (coh co + coh cod (inhin inh in d (v (co in d + (in + cod (vi (d d/( A. An elecroaic poenial v i given b he funcion v(, = ep( /λ in(k i.e., i deca eponeniall along he ai and i periodic along he ai. (a Wrie down he oal differenial of v(,. (b Show ha 2 v and 2 v are equal remember ha for eample on he boom of a parial differenial mean ha we ake he derivaive wih repec o fir and hen ake he derivaive wih repec. 5B. The heigh h of each poin (, of an area of land i given b h(, = a( a 2 where a i a poiive conan. Find he locaion and heigh of he highe and lowe poin of he errain, and alo hoe along he and ae. Skech a map of he region b howing conour of conan h in he (, plane. 6B. Find du d in wo wa given ha (i u = n n and = coa, = in b, where a, b and n are conan, (ii u = and = ln

8 CHAPTER 5. PARTIAL DERIVATIVES 55 7B. The urface of a piece of ound-damping maerial undulae in boh he and direcion. The heigh of he urface of he maerial i decribed b an equaion which give he heigh h a a funcion of he and coordinae. Thi funcion i h(, = co(k co(k (a Calculae he wo parial derivaive of h. Now, if we move acro hi urface a a veloci v = (v, v hen a a ime our and coordinae are given b = v = v (b Uing he parial derivaive ou calculaed in a, find he derivaive dh/d which give he rae of change of he heigh a we move acro he urface a he veloci v. Wrie our anwer a a funcion onl of, no of and. 8C. For f(, = e, find /, and /. Check ha ( / (/ = ( / (/. Find (/ r θ and (/ θ r (i uing he chain rule, (ii b fir epreing f in erm of polar coordinae r, θ, and check ha he wo mehod give he ame reul. 9A. If z z 5 = 0 (an implici equaion for an of he variable,, z in erm of he oher wo, find, z, and how ha heir produc i 1. 10A. Van der Waal equaion (p + a/v 2 (V b = RT i an earl (and in man wa remarkabl ucceful aemp o repreen he relaion beween he preure p, volume V and emperaure T of a real ga (R, a, b are conan for a given ma of ga. Calculae epreion for p V, V T T p, T p, and verif heir produc i 1. V 11B. f(, i a calar funcion of poiion on he plane. Poiion ma alo be pecified b Careian coordinae u, v which are referred o ae roaed b an angle θ from he and aie. Show ha f 2 = 2 f u f v 2, i.e. he 2 dimenional 2 operaor i invarian under roaion of ae. 12A. Show ha V = (Ar n + Br n co(nθ + ǫ, where A, B, n and ǫ are arbirar conan, aifie he equaion 2 V r V r r V r 2 θ 2 = 0

9 CHAPTER 5. PARTIAL DERIVATIVES 56 13A. If V = f( c + g( + c, where f and g are arbirar funcion, and c i a conan, prove ha 2 V V c 2 2 = 0 14C. If u = +, v =, and f i a funcion of and, epre prove ha = 2 f u 2 + u 2 f u v + f v 2 c + v, in erm of u, v and 15C. The independen variable, are ranformed ino new variable X, Y given b he equaion X =, Y = 1/. If a funcion f(, i hu ranformed ino F(X, Y hen calculae F X and F Y in erm of and. 16B. If f i a funcion of and which can, uing he ubiuion = re θ, = re θ, be wrien a a funcion of r and θ how ha 2 = r r + θ, 2 = r r θ. 17B. Find a Talor epanion up o quadraic erm in 2 and 3 of f(, = e abou he poin = 2, = 3. 18B. Find he aionar value of he funcion (a ( (b inin (0 < < π,0 < < π (c ( e and deermine heir characer. 19B. (a Find he aionar poin of he funcion z = ( 2 2 e 2 2. (b Find he conour on which z = 0 and eamine he behaviour of z on he ae. Hence, or oherwie, deermine he characer of he aionar poin. Skech he conour. 20B. For he funcion f(, = ( find he componen of he vecor (/, /, known a he gradien vecor, a he poin ( 1, 0, (1, 0, ( 1, 1 and (1, 1. Make a kech howing he direcion of he gradien vecor a hee poin. 21B. Show ha f(, = ( ha aionar value a (0, 0 and (1/3, 1/3 and inveigae heir naure. 22C. A aionar poin of he funcion f(, i a minimum if he Heian mari (i.e. he mari of econd derivaive i poiive definie (i.e. i eigenvalue are boh poiive and a addle if he eigenvalue have oppoie ign. Inveigae he aionar poin of f(, =

10 CHAPTER 5. PARTIAL DERIVATIVES 57 Anwer o Chaper 5 Problem Noe: ou mu aemp he problem before referring o he anwer 1. (a (b (c (d = 1 = co( in( = e (+ 1 (+ 2 = ( (a + = (b + = 0 (c + = 2 dg(u du u= 3. Noe here f(, = K olve he equaion in general (i Eac, f(, =. (ii No eac. (iii Eac, f(, = (iv Eac, f(, = coh in + inhco. (v No eac. (vi Eac, f(, = arcan = arcan 4. (a dv = 1 λ e /λ in(kd + e /λ k co(kd (b = e /λ k co(k λ 5. Saionar poin a (, = (a/ 2, a/ 2 heigh 1/ 2, and ( a/ 2, a/ 2 heigh 1/ 2 6. (i du d = con 1 (ain m 1 (b(bm co(aco(b an in(ain(b (ii du d = ln ln 2 7. (a h h = k co(kin(k, = k co(kin(k (b dh d = h d d + h d d = k co(kv in(kv v k co(kv in(kv v 8. = e, = e, 2 f = e ( 1 (i r θ = r θ + r θ = e coθ e in θ = 2r coθ inθe r2 in θ co θ r = r + r = e ( r inθ e r coθ = r 2 e r2 in θ co θ (2 in 2 θ θ 1 θ θ (ii f = e r2 in θ co θ hen differeniae o obain anwer quoed above.

11 CHAPTER 5. PARTIAL DERIVATIVES z = z z = +5z4 z+4 3 = 32 +z +5z 4 p V T = p+2ab av V 3 (V b V p = RV 3 T T p p av +2ab V = V b R 11. The new coordinae are a roaed verion of he old, i.e. u = co θ + in θ and v = in θ + coθ. Uing hi coordinae ranformaion he reul in he queion follow. 12. V r = (Anrn 1 Bnr n 1 co(nθ + ǫ 2 V r 2 = (An(n 1r n 2 + Bn(n + 1r n 2 co(nθ + ǫ 2 V θ 2 = (Ar n + Br n co(nθ + ǫ Summing hee componen a inruced produce he required reul V 2 = f ( c + g ( + c 2 V 2 = c 2 f ( c + c 2 g ( + c Summing hee componen a inruced produce he required reul. 14. = u u + v v = u u + v v F 15. X = = 2 f u u 2 X + u + 2 f u v u v + 2 f u v u v + 2 f + v2 v = 2 f u f u v + 2 f = 2 f u f u v u + 2 f v 2 v + v X F Y = Y + Y 16. Changing variable produce he reul in he queion. 17. Denoe δ = 2 and δ = 3, hen f(2 + δ, 3 + δ 3e 6 + 9e 6 δ + 7e 6 δ u v + 2 f v v 2 v + v 2 v ( 27e 6 δ e 6 δδ + 16e 6 δ (a (0, 0 Maimum

12 CHAPTER 5. PARTIAL DERIVATIVES 59 (b (π/2, π/2 Maimum (c (1, 0 Saddle, (1 ± 1/ 2, ±1/ 2 Maimum if boh + ign, Minimum if mied ign. 19. (0, 0 Saddle, (±1, 0 Maima, (0, ±1 Minima 20. Repecivel ( 1, 2, ( 1, 2, (2, 4, (2, (0, 0 Maimum, (1/3, 1/3 Saddle. 22. (0, 0 Saddle, ( 1/12, 1/6 Minimum

2. VECTORS. R Vectors are denoted by bold-face characters such as R, V, etc. The magnitude of a vector, such as R, is denoted as R, R, V

2. VECTORS. R Vectors are denoted by bold-face characters such as R, V, etc. The magnitude of a vector, such as R, is denoted as R, R, V ME 352 VETS 2. VETS Vecor algebra form he mahemaical foundaion for kinemaic and dnamic. Geomer of moion i a he hear of boh he kinemaic and dnamic of mechanical em. Vecor anali i he imehonored ool for decribing

More information

Module 2: Analysis of Stress

Module 2: Analysis of Stress Module/Leon Module : Anali of Sre.. INTRODUCTION A bod under he acion of eernal force, undergoe diorion and he effec due o hi em of force i ranmied hroughou he bod developing inernal force in i. To eamine

More information

CHAPTER 7: SECOND-ORDER CIRCUITS

CHAPTER 7: SECOND-ORDER CIRCUITS EEE5: CI RCUI T THEORY CHAPTER 7: SECOND-ORDER CIRCUITS 7. Inroducion Thi chaper conider circui wih wo orage elemen. Known a econd-order circui becaue heir repone are decribed by differenial equaion ha

More information

Linear Algebra Primer

Linear Algebra Primer Linear Algebra rimer And a video dicuion of linear algebra from EE263 i here (lecure 3 and 4): hp://ee.anford.edu/coure/ee263 lide from Sanford CS3 Ouline Vecor and marice Baic Mari Operaion Deerminan,

More information

Laplace Transform. Inverse Laplace Transform. e st f(t)dt. (2)

Laplace Transform. Inverse Laplace Transform. e st f(t)dt. (2) Laplace Tranform Maoud Malek The Laplace ranform i an inegral ranform named in honor of mahemaician and aronomer Pierre-Simon Laplace, who ued he ranform in hi work on probabiliy heory. I i a powerful

More information

ū(e )(1 γ 5 )γ α v( ν e ) v( ν e )γ β (1 + γ 5 )u(e ) tr (1 γ 5 )γ α ( p ν m ν )γ β (1 + γ 5 )( p e + m e ).

ū(e )(1 γ 5 )γ α v( ν e ) v( ν e )γ β (1 + γ 5 )u(e ) tr (1 γ 5 )γ α ( p ν m ν )γ β (1 + γ 5 )( p e + m e ). PHY 396 K. Soluion for problem e #. Problem (a: A poin of noaion: In he oluion o problem, he indice µ, e, ν ν µ, and ν ν e denoe he paricle. For he Lorenz indice, I hall ue α, β, γ, δ, σ, and ρ, bu never

More information

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms

More information

Chapter 7: Inverse-Response Systems

Chapter 7: Inverse-Response Systems Chaper 7: Invere-Repone Syem Normal Syem Invere-Repone Syem Baic Sar ou in he wrong direcion End up in he original eady-ae gain value Two or more yem wih differen magniude and cale in parallel Main yem

More information

Physics 240: Worksheet 16 Name

Physics 240: Worksheet 16 Name Phyic 4: Workhee 16 Nae Non-unifor circular oion Each of hee proble involve non-unifor circular oion wih a conan α. (1) Obain each of he equaion of oion for non-unifor circular oion under a conan acceleraion,

More information

y z P 3 P T P1 P 2. Werner Purgathofer. b a

y z P 3 P T P1 P 2. Werner Purgathofer. b a Einführung in Viual Compuing Einführung in Viual Compuing 86.822 in co T P 3 P co in T P P 2 co in Geomeric Tranformaion Geomeric Tranformaion W P h f Werner Purgahofer b a Tranformaion in he Rendering

More information

6.8 Laplace Transform: General Formulas

6.8 Laplace Transform: General Formulas 48 HAP. 6 Laplace Tranform 6.8 Laplace Tranform: General Formula Formula Name, ommen Sec. F() l{ f ()} e f () d f () l {F()} Definiion of Tranform Invere Tranform 6. l{af () bg()} al{f ()} bl{g()} Lineariy

More information

Discussion Session 2 Constant Acceleration/Relative Motion Week 03

Discussion Session 2 Constant Acceleration/Relative Motion Week 03 PHYS 100 Dicuion Seion Conan Acceleraion/Relaive Moion Week 03 The Plan Today you will work wih your group explore he idea of reference frame (i.e. relaive moion) and moion wih conan acceleraion. You ll

More information

Curvature. Institute of Lifelong Learning, University of Delhi pg. 1

Curvature. Institute of Lifelong Learning, University of Delhi pg. 1 Dicipline Coure-I Semeer-I Paper: Calculu-I Leon: Leon Developer: Chaianya Kumar College/Deparmen: Deparmen of Mahemaic, Delhi College of r and Commerce, Univeriy of Delhi Iniue of Lifelong Learning, Univeriy

More information

, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max

, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max ecure 8 7. Sabiliy Analyi For an n dimenional vecor R n, he and he vecor norm are defined a: = T = i n i (7.) I i eay o how ha hee wo norm aify he following relaion: n (7.) If a vecor i ime-dependen, hen

More information

CONTROL SYSTEMS. Chapter 10 : State Space Response

CONTROL SYSTEMS. Chapter 10 : State Space Response CONTROL SYSTEMS Chaper : Sae Space Repone GATE Objecive & Numerical Type Soluion Queion 5 [GATE EE 99 IIT-Bombay : Mark] Conider a econd order yem whoe ae pace repreenaion i of he form A Bu. If () (),

More information

Problem Set If all directed edges in a network have distinct capacities, then there is a unique maximum flow.

Problem Set If all directed edges in a network have distinct capacities, then there is a unique maximum flow. CSE 202: Deign and Analyi of Algorihm Winer 2013 Problem Se 3 Inrucor: Kamalika Chaudhuri Due on: Tue. Feb 26, 2013 Inrucion For your proof, you may ue any lower bound, algorihm or daa rucure from he ex

More information

1 CHAPTER 14 LAPLACE TRANSFORMS

1 CHAPTER 14 LAPLACE TRANSFORMS CHAPTER 4 LAPLACE TRANSFORMS 4 nroducion f x) i a funcion of x, where x lie in he range o, hen he funcion p), defined by p) px e x) dx, 4 i called he Laplace ranform of x) However, in hi chaper, where

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual

More information

(π 3)k. f(t) = 1 π 3 sin(t)

(π 3)k. f(t) = 1 π 3 sin(t) Mah 6 Fall 6 Dr. Lil Yen Tes Show all our work Name: Score: /6 No Calculaor permied in his par. Read he quesions carefull. Show all our work and clearl indicae our final answer. Use proper noaion. Problem

More information

Exponential Sawtooth

Exponential Sawtooth ECPE 36 HOMEWORK 3: PROPERTIES OF THE FOURIER TRANSFORM SOLUTION. Exponenial Sawooh: The eaie way o do hi problem i o look a he Fourier ranform of a ingle exponenial funcion, () = exp( )u(). From he able

More information

( ) 2. Review Exercise 2. cos θ 2 3 = = 2 tan. cos. 2 x = = x a. Since π π, = 2. sin = = 2+ = = cotx. 2 sin θ 2+

( ) 2. Review Exercise 2. cos θ 2 3 = = 2 tan. cos. 2 x = = x a. Since π π, = 2. sin = = 2+ = = cotx. 2 sin θ 2+ Review Eercise sin 5 cos sin an cos 5 5 an 5 9 co 0 a sinθ 6 + 4 6 + sin θ 4 6+ + 6 + 4 cos θ sin θ + 4 4 sin θ + an θ cos θ ( ) + + + + Since π π, < θ < anθ should be negaive. anθ ( + ) Pearson Educaion

More information

Linear Algebra Primer

Linear Algebra Primer Linear Algebra Primer Juan Carlo Nieble and Ranja Krihna Sanford Viion and Learning Lab Anoher, ver in-deph linear algebra review from CS229 i available here: hp://c229.anford.edu/ecion/c229-linalg.pdf

More information

Linear Motion, Speed & Velocity

Linear Motion, Speed & Velocity Add Iporan Linear Moion, Speed & Velociy Page: 136 Linear Moion, Speed & Velociy NGSS Sandard: N/A MA Curriculu Fraework (2006): 1.1, 1.2 AP Phyic 1 Learning Objecive: 3.A.1.1, 3.A.1.3 Knowledge/Underanding

More information

CHAPTER. Forced Equations and Systems { } ( ) ( ) 8.1 The Laplace Transform and Its Inverse. Transforms from the Definition.

CHAPTER. Forced Equations and Systems { } ( ) ( ) 8.1 The Laplace Transform and Its Inverse. Transforms from the Definition. CHAPTER 8 Forced Equaion and Syem 8 The aplace Tranform and I Invere Tranform from he Definiion 5 5 = b b {} 5 = 5e d = lim5 e = ( ) b {} = e d = lim e + e d b = (inegraion by par) = = = = b b ( ) ( )

More information

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

AP Calculus BC Chapter 10 Part 1 AP Exam Problems AP Calculus BC Chaper Par AP Eam Problems All problems are NO CALCULATOR unless oherwise indicaed Parameric Curves and Derivaives In he y plane, he graph of he parameric equaions = 5 + and y= for, is a

More information

ME 391 Mechanical Engineering Analysis

ME 391 Mechanical Engineering Analysis Fall 04 ME 39 Mechanical Engineering Analsis Eam # Soluions Direcions: Open noes (including course web posings). No books, compuers, or phones. An calculaor is fair game. Problem Deermine he posiion of

More information

13.1 Accelerating Objects

13.1 Accelerating Objects 13.1 Acceleraing Objec A you learned in Chaper 12, when you are ravelling a a conan peed in a raigh line, you have uniform moion. However, mo objec do no ravel a conan peed in a raigh line o hey do no

More information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow 1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering

More information

Math 2214 Solution Test 1 B Spring 2016

Math 2214 Solution Test 1 B Spring 2016 Mah 14 Soluion Te 1 B Spring 016 Problem 1: Ue eparaion of ariable o ole he Iniial alue DE Soluion (14p) e =, (0) = 0 d = e e d e d = o = ln e d uing u-du b leing u = e 1 e = + where C = for he iniial

More information

Introduction to SLE Lecture Notes

Introduction to SLE Lecture Notes Inroducion o SLE Lecure Noe May 13, 16 - The goal of hi ecion i o find a ufficien condiion of λ for he hull K o be generaed by a imple cure. I urn ou if λ 1 < 4 hen K i generaed by a imple curve. We will

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Mon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5

Mon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5 Mah 225-4 Week 2 April 2-6 coninue.-.3; alo cover par of.4-.5, EP 7.6 Mon Apr 2:.-.3 Laplace ranform and iniial value problem like we udied in Chaper 5 Announcemen: Warm-up Exercie: Recall, The Laplace

More information

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities: Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial

More information

Algorithmic Discrete Mathematics 6. Exercise Sheet

Algorithmic Discrete Mathematics 6. Exercise Sheet Algorihmic Dicree Mahemaic. Exercie Shee Deparmen of Mahemaic SS 0 PD Dr. Ulf Lorenz 7. and 8. Juni 0 Dipl.-Mah. David Meffer Verion of June, 0 Groupwork Exercie G (Heap-Sor) Ue Heap-Sor wih a min-heap

More information

EE202 Circuit Theory II

EE202 Circuit Theory II EE202 Circui Theory II 2017-2018, Spring Dr. Yılmaz KALKAN I. Inroducion & eview of Fir Order Circui (Chaper 7 of Nilon - 3 Hr. Inroducion, C and L Circui, Naural and Sep epone of Serie and Parallel L/C

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Randomized Perfect Bipartite Matching

Randomized Perfect Bipartite Matching Inenive Algorihm Lecure 24 Randomized Perfec Biparie Maching Lecurer: Daniel A. Spielman April 9, 208 24. Inroducion We explain a randomized algorihm by Ahih Goel, Michael Kapralov and Sanjeev Khanna for

More information

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES PROBLEMS FOR MATH 6 If a problem is sarred, all subproblems are due. If onl subproblems are sarred, onl hose are due. 00. Shor answer quesions. SLOPES OF TANGENT LINES (a) A ball is hrown ino he air. Is

More information

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems Sample Final Exam Covering Chaper 9 (final04) Sample Final Exam (final03) Covering Chaper 9 of Fundamenal of Signal & Syem Problem (0 mar) Conider he caual opamp circui iniially a re depiced below. I LI

More information

Introduction to Congestion Games

Introduction to Congestion Games Algorihmic Game Theory, Summer 2017 Inroducion o Congeion Game Lecure 1 (5 page) Inrucor: Thoma Keelheim In hi lecure, we ge o know congeion game, which will be our running example for many concep in game

More information

Chapter 6. Laplace Transforms

Chapter 6. Laplace Transforms Chaper 6. Laplace Tranform Kreyzig by YHLee;45; 6- An ODE i reduced o an algebraic problem by operaional calculu. The equaion i olved by algebraic manipulaion. The reul i ranformed back for he oluion of

More information

1 Motivation and Basic Definitions

1 Motivation and Basic Definitions CSCE : Deign and Analyi of Algorihm Noe on Max Flow Fall 20 (Baed on he preenaion in Chaper 26 of Inroducion o Algorihm, 3rd Ed. by Cormen, Leieron, Rive and Sein.) Moivaion and Baic Definiion Conider

More information

EE Control Systems LECTURE 2

EE Control Systems LECTURE 2 Copyrigh F.L. Lewi 999 All righ reerved EE 434 - Conrol Syem LECTURE REVIEW OF LAPLACE TRANSFORM LAPLACE TRANSFORM The Laplace ranform i very ueful in analyi and deign for yem ha are linear and ime-invarian

More information

NEUTRON DIFFUSION THEORY

NEUTRON DIFFUSION THEORY NEUTRON DIFFUSION THEORY M. Ragheb 4//7. INTRODUCTION The diffuion heory model of neuron ranpor play a crucial role in reacor heory ince i i imple enough o allow cienific inigh, and i i ufficienly realiic

More information

5.2 GRAPHICAL VELOCITY ANALYSIS Polygon Method

5.2 GRAPHICAL VELOCITY ANALYSIS Polygon Method ME 352 GRHICL VELCITY NLYSIS 52 GRHICL VELCITY NLYSIS olygon Mehod Velociy analyi form he hear of kinemaic and dynamic of mechanical yem Velociy analyi i uually performed following a poiion analyi; ie,

More information

CHAPTER 7. Definition and Properties. of Laplace Transforms

CHAPTER 7. Definition and Properties. of Laplace Transforms SERIES OF CLSS NOTES FOR 5-6 TO INTRODUCE LINER ND NONLINER PROBLEMS TO ENGINEERS, SCIENTISTS, ND PPLIED MTHEMTICINS DE CLSS NOTES COLLECTION OF HNDOUTS ON SCLR LINER ORDINRY DIFFERENTIL EQUTIONS (ODE")

More information

Chapter 6. Laplace Transforms

Chapter 6. Laplace Transforms 6- Chaper 6. Laplace Tranform 6.4 Shor Impule. Dirac Dela Funcion. Parial Fracion 6.5 Convoluion. Inegral Equaion 6.6 Differeniaion and Inegraion of Tranform 6.7 Syem of ODE 6.4 Shor Impule. Dirac Dela

More information

Instrumentation & Process Control

Instrumentation & Process Control Chemical Engineering (GTE & PSU) Poal Correpondence GTE & Public Secor Inrumenaion & Proce Conrol To Buy Poal Correpondence Package call a -999657855 Poal Coure ( GTE & PSU) 5 ENGINEERS INSTITUTE OF INDI.

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

DEPARTMENT OF ECONOMICS /11. dy =, for each of the following, use the chain rule to find dt

DEPARTMENT OF ECONOMICS /11. dy =, for each of the following, use the chain rule to find dt SCHOO OF ORIENTA AND AFRICAN STUDIES UNIVERSITY OF ONDON DEPARTMENT OF ECONOMICS 14 15 1/11-15 16 MSc Economics PREIMINARY MATHEMATICS EXERCISE 4 (Skech answer) Course websie: hp://mercur.soas.ac.uk/users/sm97/eaching_msc_premah.hm

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15. SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a

More information

Rectilinear Kinematics

Rectilinear Kinematics Recilinear Kinemaic Coninuou Moion Sir Iaac Newon Leonard Euler Oeriew Kinemaic Coninuou Moion Erraic Moion Michael Schumacher. 7-ime Formula 1 World Champion Kinemaic The objecie of kinemaic i o characerize

More information

a. Show that these lines intersect by finding the point of intersection. b. Find an equation for the plane containing these lines.

a. Show that these lines intersect by finding the point of intersection. b. Find an equation for the plane containing these lines. Mah A Final Eam Problems for onsideraion. Show all work for credi. Be sure o show wha you know. Given poins A(,,, B(,,, (,, 4 and (,,, find he volume of he parallelepiped wih adjacen edges AB, A, and A.

More information

Admin MAX FLOW APPLICATIONS. Flow graph/networks. Flow constraints 4/30/13. CS lunch today Grading. in-flow = out-flow for every vertex (except s, t)

Admin MAX FLOW APPLICATIONS. Flow graph/networks. Flow constraints 4/30/13. CS lunch today Grading. in-flow = out-flow for every vertex (except s, t) /0/ dmin lunch oday rading MX LOW PPLIION 0, pring avid Kauchak low graph/nework low nework direced, weighed graph (V, ) poiive edge weigh indicaing he capaciy (generally, aume ineger) conain a ingle ource

More information

On Line Supplement to Strategic Customers in a Transportation Station When is it Optimal to Wait? A. Manou, A. Economou, and F.

On Line Supplement to Strategic Customers in a Transportation Station When is it Optimal to Wait? A. Manou, A. Economou, and F. On Line Spplemen o Sraegic Comer in a Tranporaion Saion When i i Opimal o Wai? A. Mano, A. Economo, and F. Karaemen 11. Appendix In hi Appendix, we provide ome echnical analic proof for he main rel of

More information

Let. x y. denote a bivariate time series with zero mean.

Let. x y. denote a bivariate time series with zero mean. Linear Filer Le x y : T denoe a bivariae ime erie wih zero mean. Suppoe ha he ime erie {y : T} i conruced a follow: y a x The ime erie {y : T} i aid o be conruced from {x : T} by mean of a Linear Filer.

More information

Review - Quiz # 1. 1 g(y) dy = f(x) dx. y x. = u, so that y = xu and dy. dx (Sometimes you may want to use the substitution x y

Review - Quiz # 1. 1 g(y) dy = f(x) dx. y x. = u, so that y = xu and dy. dx (Sometimes you may want to use the substitution x y Review - Quiz # 1 (1) Solving Special Tpes of Firs Order Equaions I. Separable Equaions (SE). d = f() g() Mehod of Soluion : 1 g() d = f() (The soluions ma be given implicil b he above formula. Remember,

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

1 st order ODE Initial Condition

1 st order ODE Initial Condition Mah-33 Chapers 1-1 s Order ODE Sepember 1, 17 1 1 s order ODE Iniial Condiion f, sandard form LINEAR NON-LINEAR,, p g differenial form M x dx N x d differenial form is equivalen o a pair of differenial

More information

Flow networks. Flow Networks. A flow on a network. Flow networks. The maximum-flow problem. Introduction to Algorithms, Lecture 22 December 5, 2001

Flow networks. Flow Networks. A flow on a network. Flow networks. The maximum-flow problem. Introduction to Algorithms, Lecture 22 December 5, 2001 CS 545 Flow Nework lon Efra Slide courey of Charle Leieron wih mall change by Carola Wenk Flow nework Definiion. flow nework i a direced graph G = (V, E) wih wo diinguihed verice: a ource and a ink. Each

More information

Theory of! Partial Differential Equations!

Theory of! Partial Differential Equations! hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

THE SINE INTEGRAL. x dt t

THE SINE INTEGRAL. x dt t THE SINE INTEGRAL As one learns in elemenary calculus, he limi of sin(/ as vanishes is uniy. Furhermore he funcion is even and has an infinie number of zeros locaed a ±n for n1,,3 Is plo looks like his-

More information

Theory of! Partial Differential Equations-I!

Theory of! Partial Differential Equations-I! hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4) Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion

More information

Algorithms and Data Structures 2011/12 Week 9 Solutions (Tues 15th - Fri 18th Nov)

Algorithms and Data Structures 2011/12 Week 9 Solutions (Tues 15th - Fri 18th Nov) Algorihm and Daa Srucure 2011/ Week Soluion (Tue 15h - Fri 18h No) 1. Queion: e are gien 11/16 / 15/20 8/13 0/ 1/ / 11/1 / / To queion: (a) Find a pair of ube X, Y V uch ha f(x, Y) = f(v X, Y). (b) Find

More information

13.1 Circuit Elements in the s Domain Circuit Analysis in the s Domain The Transfer Function and Natural Response 13.

13.1 Circuit Elements in the s Domain Circuit Analysis in the s Domain The Transfer Function and Natural Response 13. Chaper 3 The Laplace Tranform in Circui Analyi 3. Circui Elemen in he Domain 3.-3 Circui Analyi in he Domain 3.4-5 The Tranfer Funcion and Naural Repone 3.6 The Tranfer Funcion and he Convoluion Inegral

More information

Math 2214 Solution Test 1B Fall 2017

Math 2214 Solution Test 1B Fall 2017 Mah 14 Soluion Tes 1B Fall 017 Problem 1: A ank has a capaci for 500 gallons and conains 0 gallons of waer wih lbs of sal iniiall. A soluion conaining of 8 lbsgal of sal is pumped ino he ank a 10 galsmin.

More information

18.03SC Unit 3 Practice Exam and Solutions

18.03SC Unit 3 Practice Exam and Solutions Sudy Guide on Sep, Dela, Convoluion, Laplace You can hink of he ep funcion u() a any nice mooh funcion which i for < a and for > a, where a i a poiive number which i much maller han any ime cale we care

More information

Vector Calculus. Chapter 2

Vector Calculus. Chapter 2 Chaper Vecor Calculus. Elemenar. Vecor Produc. Differeniaion of Vecors 4. Inegraion of Vecors 5. Del Operaor or Nabla (Smbol 6. Polar Coordinaes Chaper Coninued 7. Line Inegral 8. Volume Inegral 9. Surface

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

PSAT/NMSQT PRACTICE ANSWER SHEET SECTION 3 EXAMPLES OF INCOMPLETE MARKS COMPLETE MARK B C D B C D B C D B C D B C D 13 A B C D B C D 11 A B C D B C D

PSAT/NMSQT PRACTICE ANSWER SHEET SECTION 3 EXAMPLES OF INCOMPLETE MARKS COMPLETE MARK B C D B C D B C D B C D B C D 13 A B C D B C D 11 A B C D B C D PSTNMSQT PRCTICE NSWER SHEET COMPLETE MRK EXMPLES OF INCOMPLETE MRKS I i recommended a you ue a No pencil I i very imporan a you fill in e enire circle darkly and compleely If you cange your repone, erae

More information

Notes on MRI, Part II

Notes on MRI, Part II BME 483 MRI Noe : page 1 Noe on MRI, Par II Signal Recepion in MRI The ignal ha we deec in MRI i a volage induced in an RF coil by change in agneic flu fro he preceing agneizaion in he objec. One epreion

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

Problem Set 7-7. dv V ln V = kt + C. 20. Assume that df/dt still equals = F RF. df dr = =

Problem Set 7-7. dv V ln V = kt + C. 20. Assume that df/dt still equals = F RF. df dr = = 20. Assume ha df/d sill equals = F + 0.02RF. df dr df/ d F+ 0. 02RF = = 2 dr/ d R 0. 04RF 0. 01R 10 df 11. 2 R= 70 and F = 1 = = 0. 362K dr 31 21. 0 F (70, 30) (70, 1) R 100 Noe ha he slope a (70, 1) is

More information

and v y . The changes occur, respectively, because of the acceleration components a x and a y

and v y . The changes occur, respectively, because of the acceleration components a x and a y Week 3 Reciaion: Chaper3 : Problems: 1, 16, 9, 37, 41, 71. 1. A spacecraf is raveling wih a veloci of v0 = 5480 m/s along he + direcion. Two engines are urned on for a ime of 84 s. One engine gives he

More information

u(t) Figure 1. Open loop control system

u(t) Figure 1. Open loop control system Open loop conrol v cloed loop feedbac conrol The nex wo figure preen he rucure of open loop and feedbac conrol yem Figure how an open loop conrol yem whoe funcion i o caue he oupu y o follow he reference

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k Challenge Problems DIS 03 and 0 March 6, 05 Choose one of he following problems, and work on i in your group. Your goal is o convince me ha your answer is correc. Even if your answer isn compleely correc,

More information

Kinematics in two dimensions

Kinematics in two dimensions Lecure 5 Phsics I 9.18.13 Kinemaics in wo dimensions Course websie: hp://facul.uml.edu/andri_danlo/teaching/phsicsi Lecure Capure: hp://echo36.uml.edu/danlo13/phsics1fall.hml 95.141, Fall 13, Lecure 5

More information

Motion In One Dimension. Graphing Constant Speed

Motion In One Dimension. Graphing Constant Speed Moion In One Dimenion PLATO AND ARISTOTLE GALILEO GALILEI LEANING TOWER OF PISA Graphing Conan Speed Diance v. Time for Toy Car (0-5 ec.) be-fi line (from TI calculaor) d = 207.7 12.6 Diance (cm) 1000

More information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

Math 2214 Solution Test 1A Spring 2016

Math 2214 Solution Test 1A Spring 2016 Mah 14 Soluion Tes 1A Spring 016 sec Problem 1: Wha is he larges -inerval for which ( 4) = has a guaraneed + unique soluion for iniial value (-1) = 3 according o he Exisence Uniqueness Theorem? Soluion

More information

MEI STRUCTURED MATHEMATICS 4758

MEI STRUCTURED MATHEMATICS 4758 OXFORD CAMBRIDGE AND RSA EXAMINATIONS Advanced Subsidiary General Cerificae of Educaion Advanced General Cerificae of Educaion MEI STRUCTURED MATHEMATICS 4758 Differenial Equaions Thursday 5 JUNE 006 Afernoon

More information

To become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship

To become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship Laplace Tranform (Lin & DeCarlo: Ch 3) ENSC30 Elecric Circui II The Laplace ranform i an inegral ranformaion. I ranform: f ( ) F( ) ime variable complex variable From Euler > Lagrange > Laplace. Hence,

More information

System of Linear Differential Equations

System of Linear Differential Equations Sysem of Linear Differenial Equaions In "Ordinary Differenial Equaions" we've learned how o solve a differenial equaion for a variable, such as: y'k5$e K2$x =0 solve DE yx = K 5 2 ek2 x C_C1 2$y''C7$y

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information

Applicable Mathematics 2A

Applicable Mathematics 2A Applicable Mahemaics A Lecure Noes Revised: Augus 00 Please noe ha hese are my lecure noes: hey are no course noes. So I will be following hese noes very closely, supplemened by he homework eamples ec

More information

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details! MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his

More information

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11. 1 Mah 334 Tes 1 KEY Spring 21 Secion: 1 Insrucor: Sco Glasgow Daes: Ma 1 and 11. Do NOT wrie on his problem saemen bookle, excep for our indicaion of following he honor code jus below. No credi will be

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

CHAPTER 2: Mathematics for Microeconomics

CHAPTER 2: Mathematics for Microeconomics CHAPTER : Mahemaics for Microeconomics The problems in his chaper are primarily mahemaical. They are inended o give sudens some pracice wih he conceps inroduced in Chaper, bu he problems in hemselves offer

More information

PHYSICS 151 Notes for Online Lecture #4

PHYSICS 151 Notes for Online Lecture #4 PHYSICS 5 Noe for Online Lecure #4 Acceleraion The ga pedal in a car i alo called an acceleraor becaue preing i allow you o change your elociy. Acceleraion i how fa he elociy change. So if you ar fro re

More information

MA 366 Review - Test # 1

MA 366 Review - Test # 1 MA 366 Review - Tes # 1 Fall 5 () Resuls from Calculus: differeniaion formulas, implici differeniaion, Chain Rule; inegraion formulas, inegraion b pars, parial fracions, oher inegraion echniques. (1) Order

More information

The Residual Graph. 12 Augmenting Path Algorithms. Augmenting Path Algorithm. Augmenting Path Algorithm

The Residual Graph. 12 Augmenting Path Algorithms. Augmenting Path Algorithm. Augmenting Path Algorithm Augmening Pah Algorihm Greedy-algorihm: ar wih f (e) = everywhere find an - pah wih f (e) < c(e) on every edge augmen flow along he pah repea a long a poible The Reidual Graph From he graph G = (V, E,

More information

Chapter 3 Kinematics in Two Dimensions

Chapter 3 Kinematics in Two Dimensions Chaper 3 KINEMATICS IN TWO DIMENSIONS PREVIEW Two-dimensional moion includes objecs which are moing in wo direcions a he same ime, such as a projecile, which has boh horizonal and erical moion. These wo

More information