Limits at Infinity. Limit at negative infinity. Limit at positive infinity. Definition of Limits at Infinity Let L be a real number.

Size: px
Start display at page:

Download "Limits at Infinity. Limit at negative infinity. Limit at positive infinity. Definition of Limits at Infinity Let L be a real number."

Transcription

1 0_005.qd //0 : PM Page CHAPTER Applicaions of Differeniaion f() as Secion.5 f() = + f() as The i of f as approaches or is. Figure. Limis a Infini Deermine (finie) is a infini. Deermine he horizonal asmpoes, if an, of he graph of a funcion. Deermine infinie is a infini. Limis a Infini This secion discusses he end behavior of a funcion on an infinie Consider he graph of f inerval. as shown in Figure.. Graphicall, ou can see ha he values of f appear o approach as increases wihou bound or decreases wihou bound. You can come o he same conclusions numericall, as shown in he able. decreases wihou bound. increases wihou bound. f f approaches. f approaches. NOTE or The saemen f L, means ha he i eiss and he i is equal o L. f L The able suggess ha he value of f approaches as increases wihou bound. Similarl, f approaches as decreases wihou bound. These is a infini are denoed b and f f. Limi a negaive infini Limi a posiive infini To sa ha a saemen is rue as increases wihou bound means ha for some (large) real number M, he saemen is rue for all in he inerval : > M. The following definiion uses his concep. L f() = L M f is wihin unis of L as. Figure. ε ε Definiion of Limis a Infini Le L be a real number.. The saemen f L means ha for each > 0 here eiss an M > 0 such ha f L < whenever > M.. The saemen f L means ha for each > 0 here eiss an N < 0 such ha whenever < N. f L < The definiion of a i a infini is shown in Figure.. In his figure, noe ha for a given posiive number here eiss a posiive number M such ha, for > M, he graph of f will lie beween he horizonal lines given b L and L.

2 0_005.qd //0 : PM Page 99 SECTION.5 Limis a Infini 99 EXPLORATION Use a graphing uili o graph f. Describe all he imporan feaures of he graph. Can ou find a single viewing window ha shows all of hese feaures clearl? Eplain our reasoning. Wha are he horizonal asmpoes of he graph? How far o he righ do ou have o move on he graph so ha he graph is wihin 0.00 uni of is horizonal asmpoe? Eplain our reasoning. Horizonal Asmpoes In Figure., he graph of f approaches he line L as increases wihou bound. The line L is called a horizonal asmpoe of he graph of f. Definiion of a Horizonal Asmpoe The line L is a horizonal asmpoe of he graph of f if f L or f L. Noe ha from his definiion, i follows ha he graph of a funcion of can have a mos wo horizonal asmpoes one o he righ and one o he lef. Limis a infini have man of he same properies of is discussed in Secion.. For eample, if f and g boh eis, hen and f g f g f g f g. Similar properies hold for is a. When evaluaing is a infini, he following heorem is helpful. (A proof of his heorem is given in Appendi A.) THEOREM.0 Limis a Infini If r is a posiive raional number and c is an real number, hen Furhermore, if r is defined when < 0, hen c r 0. c r 0. EXAMPLE Finding a Limi a Infini Find he i: Soluion 5. Using Theorem.0, ou can wrie Proper of is

3 0_005.qd //0 : PM Page CHAPTER Applicaions of Differeniaion EXAMPLE Finding a Limi a Infini Find he i:. Soluion Noe ha boh he numeraor and he denominaor approach infini as approaches infini. NOTE When ou encouner an indeerminae form such as he one in Eample, ou should divide he numeraor and denominaor b he highes power of in he denominaor. 5 5 f() = + is a horizonal asmpoe. Figure.5 This resuls in an indeerminae form. To resolve his problem, ou can divide, boh he numeraor and he denominaor b. Afer dividing, he i ma be evaluaed as shown. 0 0 Divide numeraor and denominaor b. Simplif. Take is of numeraor and denominaor. Appl Theorem.0. So, he line is a horizonal asmpoe o he righ. B aking he i as, ou can see ha is also a horizonal asmpoe o he lef. The graph of he funcion is shown in Figure As increases, he graph of f moves closer and closer o he line. Figure. TECHNOLOGY You can es he reasonableness of he i found in Eample b evaluaing f for a few large posiive values of. For insance, f , f , and f 0, Anoher wa o es he reasonableness of he i is o use a graphing uili. For insance, in Figure., he graph of f is shown wih he horizonal line. Noe ha as increases, he graph of f moves closer and closer o is horizonal asmpoe.

4 0_005.qd //0 : PM Page 0 SECTION.5 Limis a Infini 0 A Comparison of Three Raional Funcions EXAMPLE Find each i. 5 a. 5 b. 5 c. The Granger Collecion Soluion In each case, aemping o evaluae he i produces he indeerminae form. a. Divide boh he numeraor and he denominaor b b. Divide boh he numeraor and he denominaor b MARIA AGNESI (78 799) Agnesi was one of a handful of women o receive credi for significan conribuions o mahemaics before he wenieh cenur. In her earl wenies, she wroe he firs e ha included boh differenial and inegral calculus. B age 0, she was an honorar member of he facul a he Universi of Bologna. c. Divide boh he numeraor and he denominaor b. 5 5 You can conclude ha he i does no eis because he numeraor increases wihou bound while he denominaor approaches. Guidelines for Finding Limis a ± of Raional Funcions. If he degree of he numeraor is less han he degree of he denominaor, hen he i of he raional funcion is 0.. If he degree of he numeraor is equal o he degree of he denominaor, hen he i of he raional funcion is he raio of he leading coefficiens.. If he degree of he numeraor is greaer han he degree of he denominaor, hen he i of he raional funcion does no eis. f() = + Use hese guidelines o check he resuls in Eample. These is seem reasonable when ou consider ha for large values of, he highes-power erm of he raional funcion is he mos influenial in deermining he i. For insance, he i as approaches infini of he funcion f() = 0 f() = 0 f has a horizonal asmpoe a 0. Figure.7 FOR FURTHER INFORMATION For more informaion on he conribuions of women o mahemaics, see he aricle Wh Women Succeed in Mahemaics b Mona Fabrican, Slvia Sviak, and Paricia Clark Kenschaf in Mahemaics Teacher. To view his aricle, go o he websie f is 0 because he denominaor overpowers he numeraor as increases or decreases wihou bound, as shown in Figure.7. The funcion shown in Figure.7 is a special case of a pe of curve sudied b he Ialian mahemaician Maria Gaeana Agnesi. The general form of his funcion is f 8a a Wich of Agnesi and, hrough a misranslaion of he Ialian word veréré, he curve has come o be known as he Wich of Agnesi. Agnesi s work wih his curve firs appeared in a comprehensive e on calculus ha was published in 78.

5 0_005.qd //0 : PM Page 0 0 CHAPTER Applicaions of Differeniaion In Figure.7, ou can see ha he funcion f approaches he same horizonal asmpoe o he righ and o he lef. This is alwas rue of raional funcions. Funcions ha are no raional, however, ma approach differen horizonal asmpoes o he righ and o he lef. This is demonsraed in Eample. EXAMPLE A Funcion wih Two Horizonal Asmpoes Find each i. a. b. Soluion a. For > 0, ou can wrie. So, dividing boh he numeraor and he denominaor b produces and ou can ake he i as follows. =, Horizonal asmpoe o he righ =, Horizonal asmpoe o he lef f() = + Funcions ha are no raional ma have differen righ and lef horizonal asmpoes. Figure.8 8 The horizonal asmpoe appears o be he line bu i is acuall he line. Figure.9 8 b. For < 0, ou can wrie. So, dividing boh he numeraor and he denominaor b produces and ou can ake he i as follows The graph of f is shown in Figure.8. TECHNOLOGY PITFALL If ou use a graphing uili o help esimae a i, be sure ha ou also confirm he esimae analicall he picures shown b a graphing uili can be misleading. For insance, Figure.9 shows one view of he graph of From his view, one could be convinced ha he graph has as a horizonal asmpoe. An analical approach shows ha he horizonal asmpoe is acuall. Confirm his b enlarging he viewing window on he graphing uili.

6 0_005.qd //0 : PM Page 0 SECTION.5 Limis a Infini 0 In Secion. (Eample 9), ou saw how he Squeeze Theorem can be used o evaluae is involving rigonomeric funcions. This heorem is also valid for is a infini. EXAMPLE 5 Limis Involving Trigonomeric Funcions = π = f() = sin sin = 0 As increases wihou bound, f approaches 0. Figure.0 Find each i. a. sin b. Soluion a. As approaches infini, he sine funcion oscillaes beween and. So, his i does no eis. b. Because sin, i follows ha for > 0, sin where 0 and 0. So, b he Squeeze Theorem, ou can obain sin 0 as shown in Figure.0. sin EXAMPLE Ogen Level in a Pond Suppose ha f measures he level of ogen in a pond, where f is he normal (unpollued) level and he ime is measured in weeks. When 0, organic wase is dumped ino he pond, and as he wase maerial oidizes, he level of ogen in he pond is f. Wha percen of he normal level of ogen eiss in he pond afer week? Afer weeks? Afer 0 weeks? Wha is he i as approaches infini? Ogen level f() (, 0.) (, 0.5) f() = 8 0 Weeks (0, 0.9) + + The level of ogen in a pond approaches he normal level of as approaches. Figure. Soluion When,, and 0, he levels of ogen are as shown. week weeks 0 weeks To find he i as approaches infini, divide he numeraor and he denominaor b o obain f f f %. 0 See Figure.. 50% 0% % 0

7 0_005.qd //0 : PM Page 0 0 CHAPTER Applicaions of Differeniaion Infinie Limis a Infini Man funcions do no approach a finie i as increases (or decreases) wihou bound. For insance, no polnomial funcion has a finie i a infini. The following definiion is used o describe he behavior of polnomial and oher funcions a infini. NOTE Deermining wheher a funcion has an infinie i a infini is useful in analzing he end behavior of is graph. You will see eamples of his in Secion. on curve skeching. Definiion of Infinie Limis a Infini Le f be a funcion defined on he inerval a,.. The saemen f means ha for each posiive number M, here is a corresponding number N > 0 such ha f > M whenever > N.. The saemen f means ha for each negaive number M, here is a corresponding number N > 0 such ha f < M whenever > N. Similar definiions can be given for he saemens f. f and EXAMPLE 7 Finding Infinie Limis a Infini f() = Figure. Find each i. a. b. Soluion a. As increases wihou bound, also increases wihou bound. So, ou can wrie. b. As decreases wihou bound, also decreases wihou bound. So, ou can wrie. The graph of f in Figure. illusraes hese wo resuls. These resuls agree wih he Leading Coefficien Tes for polnomial funcions as described in Secion P.. EXAMPLE 8 Finding Infinie Limis a Infini f() = + 9 Figure. 9 = Find each i. a. b. Soluion One wa o evaluae each of hese is is o use long division o rewrie he improper raional funcion as he sum of a polnomial and a raional funcion. a. b. The saemens above can be inerpreed as saing ha as approaches ±, he funcion f behaves like he funcion g. In Secion., ou will see ha his is graphicall described b saing ha he line is a slan asmpoe of he graph of f, as shown in Figure..

8 0_005.qd //0 : PM Page 05 SECTION.5 Limis a Infini 05 In Eercises and, describe in our own words wha he saemen means.. f. In Eercises 8, mach he funcion wih one of he graphs [(a), (b),, (d), (e), or (f)] using horizonal asmpoes as an aid. (a) (e) Eercises for Secion.5 (b) (d) (f). f. f 5. f. 7. f sin 8. Numerical and Graphical Analsis In Eercises 9, use a graphing uili o complee he able and esimae he i as approaches infini. Then use a graphing uili o graph he funcion and esimae he i graphicall. f f f f f f. f 5. f. f 5. In Eercises 5 and, find h, if possible. 5. f 5 0. (a) f 5 7 (a) (b) (b) In Eercises 7 0, find each i, if possible. 7. (a) 8. (a) (b) (a) 0. (a) 5 (b) See for worked-ou soluions o odd-numbered eercises. h f h f h f h f 5 h f h f f In Eercises, find he i sin cos.... cos sin (b) (b) 8 5 5

9 0_005.qd //0 : PM Page 0 0 CHAPTER Applicaions of Differeniaion In Eercises 5 8, use a graphing uili o graph he funcion and idenif an horizonal asmpoes. 5.. f f 7. f 8. In Eercises 9 and 0, find he i. Hin: Le / and find he i as sin 0. In Eercises, find he i. (Hin: Trea he epression as a fracion whose denominaor is, and raionalize he numeraor.) Use a graphing uili o verif our resul Numerical, Graphical, and Analic Analsis In Eercises 7 50, use a graphing uili o complee he able and esimae he i as approaches infini. Then use a graphing uili o graph he funcion and esimae he i. Finall, find he i analicall and compare our resuls wih he esimaes. f f 8. f 9. f sin Wriing Abou Conceps f 9 an f 5. The graph of a funcion f is shown below. To prin an enlarged cop of he graph, go o he websie f (a) Skech f. (b) Use he graphs o esimae f and f. Eplain he answers ou gave in par (b). Wriing Abou Conceps (coninued) 5. Skech a graph of a differeniable funcion f ha saisfies he following condiions and has as is onl criical number. f < 0 for < f f 5. Is i possible o skech a graph of a funcion ha saisfies he condiions of Eercise 5 and has no poins of inflecion? Eplain. 5. If f is a coninuous funcion such ha f 5, find, if possible, f for each specified condiion. (a) The graph of f is smmeric o he -ais. (b) The graph of f is smmeric o he origin. In Eercises 55 7, skech he graph of he funcion using erema, inerceps, smmer, and asmpoes. Then use a graphing uili o verif our resul f > 0 for > In Eercises 7 8, use a compuer algebra ssem o analze he graph of he funcion. Label an erema and/or asmpoes ha eis. f 7. f f 7. f 77. f f 80. g 8. g sin, > 8. f f sin

10 0_005.qd //0 : PM Page 07 SECTION.5 Limis a Infini 07 In Eercises 8 and 8, (a) use a graphing uili o graph f and g in he same viewing window, (b) verif algebraicall ha f and g represen he same funcion, and zoom ou sufficienl far so ha he graph appears as a line. Wha equaion does his line appear o have? (Noe ha he poins a which he funcion is no coninuous are no readil seen when ou zoom ou.) f f g 85. Average Cos A business has a cos of C for producing unis. The average cos per uni is C C. Find he i of C as approaches infini. 8. Engine Efficienc The efficienc of an inernal combusion engine is Efficienc where v v is he raio of he uncompressed gas o he compressed gas and c is a posiive consan dependen on he engine design. Find he i of he efficienc as he compression raio approaches infini. 87. Phsics Newon s Firs Law of Moion and Einsein s Special Theor of Relaivi differ concerning a paricle s behavior as is veloci approaches he speed of ligh, c. Funcions N and E represen he prediced veloci, v, wih respec o ime,, for a paricle acceleraed b a consan force. Wrie a i saemen ha describes each heor. c v 88. Temperaure The graph shows he emperaure T, in degrees Fahrenhei, of an apple pie seconds afer i is removed from an oven and placed on a cooling rack. 7 T (0, 5) % 00 v v c N (a) Find T. Wha does his i represen? 0 (b) Find Wha does his i represen? T. E g 89. Modeling Daa The able shows he world record imes for running mile, where represens he ear, wih 0 corresponding o 900, and is he ime in minues and seconds. A model for he daa is where he seconds have been changed o decimal pars of a minue. (a) Use a graphing uili o plo he daa and graph he model. (b) Does here appear o be a iing ime for running mile? Eplain. 90. Modeling Daa The average ping speeds S (words per minue) of a ping suden afer weeks of lessons are shown in he able. S A model for he daa is S 00 > 0. 5, (a) Use a graphing uili o plo he daa and graph he model. (b) Does here appear o be a iing ping speed? Eplain. 9. Modeling Daa A hea probe is aached o he hea echanger of a heaing ssem. The emperaure T (degrees Celsius) is recorded seconds afer he furnace is sared. The resuls for he firs minues are recorded in he able. T T 5 5 :0. :07. :0. : :5.5 :5. :8.9 :. : (a) Use he regression capabiliies of a graphing uili o find a model of he form T a b c for he daa. (b) Use a graphing uili o graph T. 5 8 A raional model for he daa is T. Use a 58 graphing uili o graph he model. (d) Find T 0 and T 0. (e) Find T. (f) Inerpre he resul in par (e) in he cone of he problem. Is i possible o do his pe of analsis using T? Eplain.

11 0_005.qd //0 : PM Page CHAPTER Applicaions of Differeniaion 9. Modeling Daa A conainer conains 5 liers of a 5% brine soluion. The able shows he concenraions C of he miure afer adding liers of a 75% brine soluion o he conainer. 9. The graph of f is shown. C ε f.5.5 C ε (a) Use he regression feaures of a graphing uili o find a model of he form C a b c for he daa. (b) Use a graphing uili o graph C. 5 A raional model for hese daa is C 0. graphing uili o graph C. Use a (d) Find C and C. Which model do ou hink bes represens he concenraion of he miure? Eplain. (e) Wha is he iing concenraion? 9. A line wih slope m passes hrough he poin 0,. (a) Wrie he disance d beween he line and he poin, as a funcion of m. (b) Use a graphing uili o graph he equaion in par (a). Find dm and dm. Inerpre he resuls m m geomericall. 9. A line wih slope m passes hrough he poin 0,. (a) Wrie he disance d beween he line and he poin, as a funcion of m. (b) Use a graphing uili o graph he equaion in par (a). Find dm and dm. Inerpre he resuls m m geomericall. 95. The graph of f is shown. ε (a) Find L f. (b) Deermine and in erms of. Deermine M, where M > 0, such ha f L < for > M. (d) Deermine N, where N < 0, such ha f L < for < N. f No drawn o scale (a) Find L f and K f. (b) Deermine and in erms of. Deermine M, where M > 0, such ha f L < for > M. (d) Deermine N, where N < 0, such ha f K < for < N. 97. Consider Use he definiion of is a. infini o find values of M ha correspond o (a) 0.5 and (b) Consider Use he definiion of is a. infini o find values of N ha correspond o (a) 0.5 and (b) 0.. In Eercises 99 0, use he definiion of is a infini o prove he i Prove ha if p a n n... a a 0 and q b m m... b b 0 a n 0, b m 0, hen 0, p a n, q b m ±, n < m n m. n > m No drawn o scale Use he definiion of infinie is a infini o prove ha. True or False? In Eercises 05 and 0, deermine wheher he saemen is rue or false. If i is false, eplain wh or give an eample ha shows i is false. 05. If f > 0 for all real numbers, hen f increases wihou bound. 0. If f < 0 for all real numbers, hen f decreases wihou bound.

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

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

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

Review Exercises for Chapter 3

Review Exercises for Chapter 3 60_00R.qd //0 :9 M age CHATER Applicaions of Differeniaion Review Eercises for Chaper. Give he definiion of a criical number, and graph a funcion f showing he differen pes of criical numbers.. Consider

More information

10.6 Parametric Equations

10.6 Parametric Equations 0_006.qd /8/05 9:05 AM Page 77 Secion 0.6 77 Parameric Equaions 0.6 Parameric Equaions Wha ou should learn Evaluae ses of parameric equaions for given values of he parameer. Skech curves ha are represened

More information

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du.

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du. MATH 3B: MIDTERM REVIEW JOE HUGHES. Inegraion by Pars. Evaluae 3 e. Soluion: Firs make he subsiuion u =. Then =, hence 3 e = e = ue u Now inegrae by pars o ge ue u = ue u e u + C and subsiue he definiion

More information

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

Sections 2.2 & 2.3 Limit of a Function and Limit Laws Mah 80 www.imeodare.com Secions. &. Limi of a Funcion and Limi Laws In secion. we saw how is arise when we wan o find he angen o a curve or he velociy of an objec. Now we urn our aenion o is in general

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

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180 Algebra Chapers & : Trigonomeric Funcions of Angles and Real Numbers Chapers & : Trigonomeric Funcions of Angles and Real Numbers - Angle Measures Radians: - a uni (rad o measure he size of an angle. rad

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

10.1 EXERCISES. y 2 t 2. y 1 t y t 3. y e

10.1 EXERCISES. y 2 t 2. y 1 t y t 3. y e 66 CHAPTER PARAMETRIC EQUATINS AND PLAR CRDINATES SLUTIN We use a graphing device o produce he graphs for he cases a,,.5,.,,.5,, and shown in Figure 7. Noice ha all of hese curves (ecep he case a ) have

More information

Second-Order Differential Equations

Second-Order Differential Equations WWW Problems and Soluions 3.1 Chaper 3 Second-Order Differenial Equaions Secion 3.1 Springs: Linear and Nonlinear Models www m Problem 3. (NonlinearSprings). A bod of mass m is aached o a wall b means

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

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

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

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

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

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

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

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

More information

5.2. The Natural Logarithm. Solution

5.2. The Natural Logarithm. Solution 5.2 The Naural Logarihm The number e is an irraional number, similar in naure o π. Is non-erminaing, non-repeaing value is e 2.718 281 828 59. Like π, e also occurs frequenly in naural phenomena. In fac,

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

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

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx. . Use Simpson s rule wih n 4 o esimae an () +. Soluion: Since we are using 4 seps, 4 Thus we have [ ( ) f() + 4f + f() + 4f 3 [ + 4 4 6 5 + + 4 4 3 + ] 5 [ + 6 6 5 + + 6 3 + ]. 5. Our funcion is f() +.

More information

5.1 - Logarithms and Their Properties

5.1 - Logarithms and Their Properties Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We

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

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

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

SPH3U: Projectiles. Recorder: Manager: Speaker:

SPH3U: Projectiles. Recorder: Manager: Speaker: SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0

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

Exponential and Logarithmic Functions -- ANSWERS -- Logarithms Practice Diploma ANSWERS 1

Exponential and Logarithmic Functions -- ANSWERS -- Logarithms Practice Diploma ANSWERS 1 Eponenial and Logarihmic Funcions -- ANSWERS -- Logarihms racice Diploma ANSWERS www.puremah.com Logarihms Diploma Syle racice Eam Answers. C. D 9. A 7. C. A. C. B 8. D. D. C NR. 8 9. C 4. C NR. NR 6.

More information

Elementary Differential Equations and Boundary Value Problems

Elementary Differential Equations and Boundary Value Problems Elemenar Differenial Equaions and Boundar Value Problems Boce. & DiPrima 9 h Ediion Chaper 1: Inroducion 1006003 คณ ตศาสตร ว ศวกรรม 3 สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา 1/2555 ผศ.ดร.อร ญญา ผศ.ดร.สมศ

More information

Section 4.4 Logarithmic Properties

Section 4.4 Logarithmic Properties Secion. Logarihmic Properies 5 Secion. Logarihmic Properies In he previous secion, we derived wo imporan properies of arihms, which allowed us o solve some asic eponenial and arihmic equaions. Properies

More information

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures.

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures. HOMEWORK # 2: MATH 2, SPRING 25 TJ HITCHMAN Noe: This is he las soluion se where I will describe he MATLAB I used o make my picures.. Exercises from he ex.. Chaper 2.. Problem 6. We are o show ha y() =

More information

Section 4.4 Logarithmic Properties

Section 4.4 Logarithmic Properties Secion. Logarihmic Properies 59 Secion. Logarihmic Properies In he previous secion, we derived wo imporan properies of arihms, which allowed us o solve some asic eponenial and arihmic equaions. Properies

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

Chapter 7: Solving Trig Equations

Chapter 7: Solving Trig Equations Haberman MTH Secion I: The Trigonomeric Funcions Chaper 7: Solving Trig Equaions Le s sar by solving a couple of equaions ha involve he sine funcion EXAMPLE a: Solve he equaion sin( ) The inverse funcions

More information

1998 Calculus AB Scoring Guidelines

1998 Calculus AB Scoring Guidelines AB{ / BC{ 1999. The rae a which waer ows ou of a pipe, in gallons per hour, is given by a diereniable funcion R of ime. The able above shows he rae as measured every hours for a {hour period. (a) Use a

More information

72 Calculus and Structures

72 Calculus and Structures 72 Calculus and Srucures CHAPTER 5 DISTANCE AND ACCUMULATED CHANGE Calculus and Srucures 73 Copyrigh Chaper 5 DISTANCE AND ACCUMULATED CHANGE 5. DISTANCE a. Consan velociy Le s ake anoher look a Mary s

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,

More information

Be able to sketch a function defined parametrically. (by hand and by calculator)

Be able to sketch a function defined parametrically. (by hand and by calculator) Pre Calculus Uni : Parameric and Polar Equaions (7) Te References: Pre Calculus wih Limis; Larson, Hoseler, Edwards. B he end of he uni, ou should be able o complee he problems below. The eacher ma provide

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page Assignmen 1 MATH 2270 SOLUTION Please wrie ou complee soluions for each of he following 6 problems (one more will sill be added). You may, of course, consul wih your classmaes, he exbook or oher resources,

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

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Math 115 Final Exam December 14, 2017

Math 115 Final Exam December 14, 2017 On my honor, as a suden, I have neiher given nor received unauhorized aid on his academic work. Your Iniials Only: Iniials: Do no wrie in his area Mah 5 Final Exam December, 07 Your U-M ID # (no uniqname):

More information

4.1 - Logarithms and Their Properties

4.1 - Logarithms and Their Properties Chaper 4 Logarihmic Funcions 4.1 - Logarihms and Their Properies Wha is a Logarihm? We define he common logarihm funcion, simply he log funcion, wrien log 10 x log x, as follows: If x is a posiive number,

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

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information

Math 1b. Calculus, Series, and Differential Equations. Final Exam Solutions

Math 1b. Calculus, Series, and Differential Equations. Final Exam Solutions Mah b. Calculus, Series, and Differenial Equaions. Final Exam Soluions Spring 6. (9 poins) Evaluae he following inegrals. 5x + 7 (a) (x + )(x + ) dx. (b) (c) x arcan x dx x(ln x) dx Soluion. (a) Using

More information

1. Kinematics I: Position and Velocity

1. Kinematics I: Position and Velocity 1. Kinemaics I: Posiion and Velociy Inroducion The purpose of his eperimen is o undersand and describe moion. We describe he moion of an objec by specifying is posiion, velociy, and acceleraion. In his

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

Cosumnes River College Principles of Macroeconomics Problem Set 1 Due January 30, 2017

Cosumnes River College Principles of Macroeconomics Problem Set 1 Due January 30, 2017 Spring 0 Cosumnes River College Principles of Macroeconomics Problem Se Due Januar 0, 0 Name: Soluions Prof. Dowell Insrucions: Wrie he answers clearl and concisel on hese shees in he spaces provided.

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

ES.1803 Topic 22 Notes Jeremy Orloff

ES.1803 Topic 22 Notes Jeremy Orloff ES.83 Topic Noes Jeremy Orloff Fourier series inroducion: coninued. Goals. Be able o compue he Fourier coefficiens of even or odd periodic funcion using he simplified formulas.. Be able o wrie and graph

More information

Motion along a Straight Line

Motion along a Straight Line chaper 2 Moion along a Sraigh Line verage speed and average velociy (Secion 2.2) 1. Velociy versus speed Cone in he ebook: fer Eample 2. Insananeous velociy and insananeous acceleraion (Secions 2.3, 2.4)

More information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species

More information

4.3 Trigonometry Extended: The Circular Functions

4.3 Trigonometry Extended: The Circular Functions 8 CHAPTER Trigonomeric Funcions. Trigonomer Eended: The Circular Funcions Wha ou ll learn abou Trigonomeric Funcions of An Angle Trigonomeric Funcions of Real Numbers Periodic Funcions The 6-Poin Uni Circle...

More information

15. Bicycle Wheel. Graph of height y (cm) above the axle against time t (s) over a 6-second interval. 15 bike wheel

15. Bicycle Wheel. Graph of height y (cm) above the axle against time t (s) over a 6-second interval. 15 bike wheel 15. Biccle Wheel The graph We moun a biccle wheel so ha i is free o roae in a verical plane. In fac, wha works easil is o pu an exension on one of he axles, and ge a suden o sand on one side and hold he

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

Section 7.4 Modeling Changing Amplitude and Midline

Section 7.4 Modeling Changing Amplitude and Midline 488 Chaper 7 Secion 7.4 Modeling Changing Ampliude and Midline While sinusoidal funcions can model a variey of behaviors, i is ofen necessary o combine sinusoidal funcions wih linear and exponenial curves

More information

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation Hea (iffusion) Equaion erivaion of iffusion Equaion The fundamenal mass balance equaion is I P O L A ( 1 ) where: I inpus P producion O oupus L losses A accumulaion Assume ha no chemical is produced or

More information

4.6 One Dimensional Kinematics and Integration

4.6 One Dimensional Kinematics and Integration 4.6 One Dimensional Kinemaics and Inegraion When he acceleraion a( of an objec is a non-consan funcion of ime, we would like o deermine he ime dependence of he posiion funcion x( and he x -componen of

More information

, where P is the number of bears at time t in years. dt (a) If 0 100, lim Pt. Is the solution curve increasing or decreasing?

, where P is the number of bears at time t in years. dt (a) If 0 100, lim Pt. Is the solution curve increasing or decreasing? CALCULUS BC WORKSHEET 1 ON LOGISTIC GROWTH Work he following on noebook paper. Use your calculaor on 4(b) and 4(c) only. 1. Suppose he populaion of bears in a naional park grows according o he logisic

More information

4.5 Constant Acceleration

4.5 Constant Acceleration 4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),

More information

INDEX. Transient analysis 1 Initial Conditions 1

INDEX. Transient analysis 1 Initial Conditions 1 INDEX Secion Page Transien analysis 1 Iniial Condiions 1 Please inform me of your opinion of he relaive emphasis of he review maerial by simply making commens on his page and sending i o me a: Frank Mera

More information

A. Using Newton s second law in one dimension, F net. , write down the differential equation that governs the motion of the block.

A. Using Newton s second law in one dimension, F net. , write down the differential equation that governs the motion of the block. Simple SIMPLE harmonic HARMONIC moion MOTION I. Differenial equaion of moion A block is conneced o a spring, one end of which is aached o a wall. (Neglec he mass of he spring, and assume he surface is

More information

MA Study Guide #1

MA Study Guide #1 MA 66 Su Guide #1 (1) Special Tpes of Firs Order Equaions I. Firs Order Linear Equaion (FOL): + p() = g() Soluion : = 1 µ() [ ] µ()g() + C, where µ() = e p() II. Separable Equaion (SEP): dx = h(x) g()

More information

The equation to any straight line can be expressed in the form:

The equation to any straight line can be expressed in the form: Sring Graphs Par 1 Answers 1 TI-Nspire Invesigaion Suden min Aims Deermine a series of equaions of sraigh lines o form a paern similar o ha formed by he cables on he Jerusalem Chords Bridge. Deermine he

More information

Instructor: Barry McQuarrie Page 1 of 5

Instructor: Barry McQuarrie Page 1 of 5 Procedure for Solving radical equaions 1. Algebraically isolae one radical by iself on one side of equal sign. 2. Raise each side of he equaion o an appropriae power o remove he radical. 3. Simplify. 4.

More information

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B) SCORING GUIDELINES (Form B) Quesion A blood vessel is 6 millimeers (mm) long Disance wih circular cross secions of varying diameer. x (mm) 6 8 4 6 Diameer The able above gives he measuremens of he B(x)

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

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

MATH 351 Solutions: TEST 3-B 23 April 2018 (revised)

MATH 351 Solutions: TEST 3-B 23 April 2018 (revised) MATH Soluions: TEST -B April 8 (revised) Par I [ ps each] Each of he following asserions is false. Give an eplici couner-eample o illusrae his.. If H: (, ) R is coninuous, hen H is unbounded. Le H() =

More information

y = (y 1)*(y 3) t

y = (y 1)*(y 3) t MATH 66 SPR REVIEW DEFINITION OF SOLUTION A funcion = () is a soluion of he differenial equaion d=d = f(; ) on he inerval ff < < fi if (d=d)() =f(; ()) for each so ha ff

More information

5 Differential Equations

5 Differential Equations Differenial Equaions. Slope Fields and Euler s Mehod. Growh and Deca. Separaion of Variables. The Logisic Equaion Sailing (Eercise 7, p. 9) Cooe Populaion (Eample, p. 7) Elk Populaion (Eample 6, p. 99)

More information

Math 116 Second Midterm March 21, 2016

Math 116 Second Midterm March 21, 2016 Mah 6 Second Miderm March, 06 UMID: EXAM SOLUTIONS Iniials: Insrucor: Secion:. Do no open his exam unil you are old o do so.. Do no wrie your name anywhere on his exam. 3. This exam has pages including

More information

Answers to Algebra 2 Unit 3 Practice

Answers to Algebra 2 Unit 3 Practice Answers o Algebra 2 Uni 3 Pracice Lesson 14-1 1. a. 0, w, 40; (0, 40); {w w, 0, w, 40} 9. a. 40,000 V Volume c. (27, 37,926) d. 27 unis 2 a. h, 30 2 2r V pr 2 (30 2 2r) c. in. d. 3,141.93 in. 2 20 40 Widh

More information

TEACHER NOTES MATH NSPIRED

TEACHER NOTES MATH NSPIRED Naural Logarihm Mah Objecives Sudens will undersand he definiion of he naural logarihm funcion in erms of a definie inegral. Sudens will be able o use his definiion o relae he value of he naural logarihm

More information

1.6. Slopes of Tangents and Instantaneous Rate of Change

1.6. Slopes of Tangents and Instantaneous Rate of Change 1.6 Slopes of Tangens and Insananeous Rae of Change When you hi or kick a ball, he heigh, h, in meres, of he ball can be modelled by he equaion h() 4.9 2 v c. In his equaion, is he ime, in seconds; c represens

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

AP CALCULUS AB/CALCULUS BC 2016 SCORING GUIDELINES. Question 1. 1 : estimate = = 120 liters/hr

AP CALCULUS AB/CALCULUS BC 2016 SCORING GUIDELINES. Question 1. 1 : estimate = = 120 liters/hr AP CALCULUS AB/CALCULUS BC 16 SCORING GUIDELINES Quesion 1 (hours) R ( ) (liers / hour) 1 3 6 8 134 119 95 74 7 Waer is pumped ino a ank a a rae modeled by W( ) = e liers per hour for 8, where is measured

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

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

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem) Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =

More information

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal?

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal? EE 35 Noes Gürdal Arslan CLASS (Secions.-.2) Wha is a signal? In his class, a signal is some funcion of ime and i represens how some physical quaniy changes over some window of ime. Examples: velociy of

More information

Math 105 Second Midterm March 16, 2017

Math 105 Second Midterm March 16, 2017 Mah 105 Second Miderm March 16, 2017 UMID: Insrucor: Iniials: Secion: 1. Do no open his exam unil you are old o do so. 2. Do no wrie your name anywhere on his exam. 3. This exam has 9 pages including his

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

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

The Fundamental Theorems of Calculus

The Fundamental Theorems of Calculus FunamenalTheorems.nb 1 The Funamenal Theorems of Calculus You have now been inrouce o he wo main branches of calculus: ifferenial calculus (which we inrouce wih he angen line problem) an inegral calculus

More information

3.6 Derivatives as Rates of Change

3.6 Derivatives as Rates of Change 3.6 Derivaives as Raes of Change Problem 1 John is walking along a sraigh pah. His posiion a he ime >0 is given by s = f(). He sars a =0from his house (f(0) = 0) and he graph of f is given below. (a) Describe

More information

Constructing Musical Scales Espen Slettnes

Constructing Musical Scales Espen Slettnes Berkele Mah Circle Sepember, 08 Inervals Consrucing Musical Scales Espen Slenes Definiion. A pure wave is a sound wave of he form = A sin (f ( + c)), where A is he ampliude and f is he pich of he wave.

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

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs. Physics 180A Fall 2008 Tes 1-120 poins Name Provide he bes answer o he following quesions and problems. Wach your sig figs. 1) The number of meaningful digis in a number is called he number of. When numbers

More information

Check in: 1 If m = 2(x + 1) and n = find y when. b y = 2m n 2

Check in: 1 If m = 2(x + 1) and n = find y when. b y = 2m n 2 7 Parameric equaions This chaer will show ou how o skech curves using heir arameric equaions conver arameric equaions o Caresian equaions find oins of inersecion of curves and lines using arameric equaions

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

Sub Module 2.6. Measurement of transient temperature

Sub Module 2.6. Measurement of transient temperature Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,

More information