Review of Vectors. Appendix A A.1 DESCRIBING THE 3D WORLD: VECTORS. 3D Coordinates. Basic Properties of Vectors: Magnitude and Direction.

Size: px
Start display at page:

Download "Review of Vectors. Appendix A A.1 DESCRIBING THE 3D WORLD: VECTORS. 3D Coordinates. Basic Properties of Vectors: Magnitude and Direction."

Transcription

1 Appendi A Review of Vectos This appendi is a summa of the mathematical aspects of vectos used in electicit and magnetism. Fo a moe detailed intoduction to vectos, see Chapte 1. A.1 DESCRIBING THE 3D WORLD: VECTORS Phsical phenomena take place in the 3D wold aound us. In ode to be able to make quantitative pedictions and give detailed, quantitative eplanations, we need tools fo descibing pecisel the positions and velocities of objects in 3D, and the changes in position and velocit due to inteactions. These tools ae mathematical entities called 3D vectos. 3D Coodinates We will use a 3D coodinate sstem to specif positions in space and othe vecto quantities. Usuall we will oient the aes of the coodinate sstem as shown in Figue A.1: + ais to the ight, + ais upwad, and + ais coming out of the page, towad ou. This is a ight-handed coodinate sstem: if ou hold the thumb, fist, and second finges of ou ight hand pependicula to each othe, and align ou thumb with the ais and ou fist finge with the ais, ou second finge points along the ais. (In some math and phsics tetbook discussions of 3D coodinate sstems, the ais points out, the ais points to the ight, and the ais points up, but we will also use a 2D coodinate sstem with up, so it makes sense alwas to have the ais point up.) Basic Popeties of Vectos: Magnitude and Diection A vecto is a quantit that has a magnitude and a diection. Fo eample, the velocit of a baseball is a vecto quantit. The magnitude of the baseball s velocit is the speed of the baseball, fo eample 20 metes/second. The diection of the baseball s velocit is the diection of its motion at a paticula instant, fo eample up o to the ight o west o in the + diection. A smbol denoting a vecto is witten with an aow ove it: Position v is a vecto. A position in space can also be consideed to be a vecto, called a position vecto, pointing fom an oigin to that location. Figue A.2 shows a position vecto that might epesent ou final position if ou stated at the oigin and walked 4 metes along the ais, then 2 metes paallel to the ais, then climbed a ladde so Figue A.1 Right-handed 3D coodinate sstem. = 3 m = 2 m = 4 m Figue A.2 A position vecto = 4, 3, 2 m and its,, and components. 1

2 2 Review of Vectos ou wee 3 metes above the gound. You new position elative to the oigin is a vecto that can be witten like this: = 4, 3, 2 m component =4m component =3m component =2m In thee dimensions a vecto is a tiple of numbes,,. Quantities like the position of an object and the velocit of an object can be epesented as vectos: = 4 m = 3 m = 2 m Figue A.3 The aow epesents the vecto = 4, 3, 2 m, dawn with its tail at location 0, 0, 2. Figue A.4 The position vecto 3, 1, 0, dawn at the oigin, in the plane. The components of the vecto specif the displacement fom the tail to the tip. The ais, which is not shown, comes out of the page, towad ou. Components of a Vecto =,, (a position vecto) 1 = 3.2, 9.2, 66.3 m (a position vecto) v = v,v,v (a velocit vecto) v 1 = 22.3, 0.4, 19.5 m/s (a velocit vecto) Each of the numbes in the tiple is efeed to as a component of the vecto. The component of the vecto v is the numbe v. The component of the vecto v 1 = 22.3, 0.4, 19.5 m/s is 19.5 m/s. A component such as v is not a vecto, since it is onl one numbe. It is impotant to note that the component of a vecto specifies the diffeence between the coodinate of the tail of the vecto and the coodinate of the tip of the vecto. It does not give an infomation about the location of the tail of the vecto (compae Figue A.2 and Figue A.3). Dawing Vectos In Figue A.2 we epesented ou position vecto elative to the oigin gaphicall b an aow whose tail is at the oigin and whose aowhead is at ou position. The length of the aow epesents the distance fom the oigin, and the diection of the aow epesents the diection of the vecto, which is the diection of a diect path fom the initial position to the final position (the displacement ; b walking and climbing ou displaced ouself fom the oigin to ou final position). Since it is difficult to daw a 3D diagam on pape, when woking on pape ou will usuall be asked to daw vectos which all lie in a single plane. Figue A.4 shows an aow in the plane epesenting the vecto 3, 1, 0. Vectos and Scalas A quantit which is epesented b a single numbe is called a scala. A scala quantit does not have a diection. Eamples include the mass of an object, such as 5 kg, o the tempeatue, such as 20C. Vectos and scalas ae ve diffeent entities; a vecto can neve be equal to a scala, and a scala cannot be added to a vecto. Scalas can be positive o negative: m =50kg T = 20 C Although a component of a vecto such as v is not a vecto, it s not a scala eithe, despite being onl one numbe. An impotant popet of a tue scala is that its value doesn t change if we oient the coodinate aes diffeentl. Rotating the aes doesn t change an object s mass, o the tempeatue, but it does change what we mean b the component of the velocit since the ais now points in a diffeent diection.

3 A.1. DESCRIBING THE 3D WORLD: VECTORS 3 Magnitude of a Vecto In Figue A.5 we again show the vecto fom Figue A.2, showing ou displacement fom the oigin. Using a 3D etension of the Pthagoean theoem fo ight tiangles (Figue A.6), the net distance ou have moved fom the stating point is (4 m)2 +(3m) 2 +(2m) 2 = 29 m = 5.39 m = 3 m = 4 m We sa that the magnitude of the position vecto is = 2 m =5.39 m The magnitude of a vecto is witten eithe with absolute-value bas aound the vecto as, o simpl b witing the smbol fo the vecto without the little aow above it,. The magnitude of a vecto can be calculated b taking the squae oot of the sum of the squaes of its components (see Figue A.6). Figue A.5 A vecto epesenting a displacement fom the oigin. MAGNITUDE OF A VECTOR If the vecto =,, then = (a scala). ( ) + 2 The magnitude of a vecto is alwas a positive numbe. The magnitude of a vecto is a single numbe, not a tiple of numbes, and it is a scala, not a vecto. The magnitude of a vecto is a tue scala, because its value doesn t change if ou otate the coodinate aes. Rotating the aes changes the individual components, but the length of the aow epesenting the vecto doesn t change. Can a Vecto be Positive o Negative? QUESTION Conside the vecto v = , 0, m/s. Is this vecto positive? Negative? Zeo? ( ) Figue A.6 The magnitude of a vecto is the squae oot of the sum of the squaes of its components (3D vesion of the Pthagoean theoem). None of these desciptions is appopiate. The component of this vecto is positive, the component is eo, and the component is negative. Vectos aen t positive, o negative, o eo. Thei components can be positive o negative o eo, but these wods just don t mean anthing when used with the vecto as a whole. On the othe hand, the magnitude of a vecto such as v is alwas positive. Mathematical Opeations Involving Vectos Although the algeba of vectos is simila to the scala algeba with which ou ae ve familia, it is not identical. Thee ae some algebaic opeations that cannot be pefomed on vectos. Algebaic opeations that ae legal fo vectos include the following opeations, which we will discuss in this chapte: adding one vecto to anothe vecto: a + w subtacting one vecto fom anothe vecto: b d finding the magnitude of a vecto: finding a unit vecto (a vecto of magnitude 1): ˆ multipling (o dividing) a vecto b a scala: 3 v o w/2 finding the ate of change of a vecto: Δ /Δt o d /dt. In late chaptes we will also see that thee ae two moe was of combining two vectos:

4 4 Review of Vectos the vecto dot poduct, whose esult is a scala the vecto coss poduct, whose esult is a vecto p 3p 2p p 1 2 p Opeations that ae Not Legal fo Vectos Although vecto algeba is simila to the odina scala algeba ou have used up to now, thee ae cetain opeations that ae not legal (and not meaningful) fo vectos: A vecto cannot be set equal to a scala. A vecto cannot be added to o subtacted fom a scala. A vecto cannot occu in the denominato of an epession. (Although ou can t divide b a vecto, note that ou can legall divide b the magnitude of a vecto, which is a scala.) Multipling a Vecto b a Scala A vecto can be multiplied (o divided) b a scala. If a vecto is multiplied b a scala, each of the components of the vecto is multiplied b the scala: If =,, then a = a, a, a 3p 2p Figue A.7 Multipling a vecto b a scala changes the magnitude of the vecto. Multipling b a negative scala eveses the diection of the vecto. If v = v,v,v then v b = v b, v b, v b ( 1 ) 6, 20, 9 = 3, 10, Multiplication b a scala scales a vecto, keeping its diection the same but making its magnitude lage o smalle (Figue A.7). Multipling b a negative scala eveses the diection of a vecto. Magnitude of a Scala You ma wonde how to find the magnitude of a quantit like 3, which involves the poduct of a scala and a vecto. This epession can be factoed: 3 = 3 The magnitude of a scala is its absolute value, so: 3 = 3 = Diection of a Vecto: Unit Vectos One wa to descibe the diection of a vecto is b specifing a unit vecto. A unit vecto is a vecto of magnitude 1, pointing in some diection. A unit vecto is witten with a hat (caet) ove it instead of an aow. The unit vecto â is called a-hat. QUESTION Is the vecto 1, 1, 1 a unit vecto? The magnitude of 1, 1, 1 is =1.73, so this is not a unit vecto. The vecto 1/ 3, 1/ 3, 1/ 3 is a unit vecto, since its magnitude is 1: ( 1 ) 2 +( 1 ) 2 +( 1 ) 2 = Note that eve component of a unit vecto must be less than o equal to 1.

5 A.1. DESCRIBING THE 3D WORLD: VECTORS 5 In ou 3D Catesian coodinate sstem, thee ae thee special unit vectos, oiented along the thee aes. The ae called i-hat, j-hat, and k-hat, and the point along the,, and aes, espectivel (Figue A.8): î= 1, 0, 0 ĵ= 0, 1, 0 ˆk = 0, 0, 1 One wa to epess a vecto is in tems of these special unit vectos: 0.02, 1.7, 30.0 =0.02î+( 1.7)ĵ+30.0ˆk We will usuall use the,, fom athe than the îĵˆk fom in this book, because the familia,, notation, used in man calculus tetbooks, emphasies that a vecto is a single entit. Not all unit vectos point along an ais, as shown in Figue A.9. Fo eample, the vectos ĝ = , , and ˆF = 0.424, 0.566, ae both unit vectos, since the magnitude of each is equal to 1. Note that eve component of a unit vecto is less than o equal to 1. k Figue A.8 The unit vectos î, ĵ, ˆk. Calculating Unit Vectos An vecto ma be factoed into the poduct of a unit vecto in the diection of the vecto, multiplied b a scala equal to the magnitude of the vecto. v = 1.5, 1.5, 0Ò m/s w = w ŵ Fo eample, a vecto of magnitude 5, aligned with the ais, could be witten as: 0, 5, 0 =5 0, 1, 0 v = 2, 2, 0Ò 2 2 Figue A.9 The unit vecto ˆv has the same diection as the vecto v, but its magnitude is 1, and it has no phsical units. Theefoe, to find a unit vecto in the diection of a paticula vecto, we just divide the vecto b its magnitude: CALCULATING A UNIT VECTOR ˆ = ( ), ˆ = =,, ( ) ( ), ( ) EXAMPLE Unit Vecto If v = 22.3, 0.4, 19.5 m/s, then ˆv = v v = 22.3, 0.4, 19.5 m/s = 0.753, , ( 22.3)2 +(0.4) 2 +( 19.5) 2 m/s Remembe that to divide a vecto b a scala, ou divide each component of the vecto b the scala. The esult is a new vecto. Note also that a unit vecto has no phsical units (such as metes pe second), because the units in the numeato and denominato cancel.

6 6 Review of Vectos Equalit of Vectos EQUALITY OF VECTORS A vecto is equal to anothe vecto if and onl if all the components of the vectos ae equal. w = means that w = and w = and w = The magnitudes and diections of two equal vectos ae the same: w = and ŵ =ˆ EXAMPLE Equal Vectos = 4, 3, 2 = ( )=5.39 ˆ = 4, 3, = 0.742, 0.557, If w = w = 4, 3, 2 w =5.39 ŵ = 0.742, 0.557, B Vecto Addition A ADDING VECTORS The sum of two vectos is anothe vecto, obtained b adding the components of the vectos. B A = A,A,A B = B,B,B A A + B = (A + B ), (A + B ), (A + B ) EXAMPLE Adding Vectos A + B B 1, 2, 3 + 4, 5, 6 = 3, 7, 9 A Figue A.10 The pocedue fo adding two vectos gaphicall: daw vectos tip to tail. To add A + B gaphicall, move B so the tail of B is at the tip of A then daw a new aow stating at the tail of A and ending at the tip of B. Waning: Don t Add Magnitudes! The magnitude of a vecto is not in geneal equal to the sum of the magnitudes of the two oiginal vectos! Fo eample, the magnitude of the vecto 3, 0, 0 is 3, and the magnitude of the vecto 2, 0, 0 is 2, but the magnitude of the vecto ( 3, 0, 0 + 2, 0, 0 ) is 1, not 5! Adding Vectos Gaphicall: Tip to Tail The sum of two vectos has a geometic intepetation. In Figue A.10 ou fist walk along displacement vecto A, followed b walking along displacement vecto B. What is ou net displacement vecto C = A + B? The component C

7 A.1. DESCRIBING THE 3D WORLD: VECTORS 7 of ou net displacement is the sum of A and B. Similal, the component C of ou net displacement is the sum of A and B. GRAPHICAL ADDITION OF VECTORS To add two vectos A and B gaphicall (Figue A.10): Daw the fist vecto A Move the second vecto B (without otating it) so its tail is located at the tip of the fist vecto Daw a new vecto fom the tail of vecto A to the tip of vecto B Vecto Subtaction The diffeence of two vectos will be ve impotant in this and subsequent chaptes. To subtact one vecto fom anothe, we subtact the components of the second fom the components of the fist: A B = (A B ), (A B ), (A B ) 1, 2, 3 4, 5, 6 = 5, 3, 3 Subtacting Vectos gaphicall: Tail to Tail To subtact one vecto B fom anothe vecto A gaphicall: Daw the fist vecto A Move the second vecto B (without otating it) so its tail is located at the tail of the fist vecto Daw a new vecto fom the tip of vecto B to the tip of vecto A Note that ou can check this algebaicall and gaphicall. As shown in Figue A.11, since the tail of A B is located at the tip of B, then the vecto A should be the sum of B and A B, as indeed it is: B +( A B)= A B A A B Figue A.11 The pocedue fo subtacting vectos gaphicall: daw vectos tail to tail; daw new vecto fom tip of second vecto to tip of fist vecto. Commutativit and Associativit Vecto addition is commutative: A + B = B + A Vecto subtaction is not commutative: A B B A The associative popet holds fo vecto addition and subtaction: The Zeo Vecto ( A + B) C = A +( B C) It is convenient to have a compact notation fo a vecto whose components ae all eo. We will use the smbol 0 to denote a eo vecto, in ode to distinguish it fom a scala quantit that has the value 0. 0 = 0, 0, 0 Fo eample, the sum of two vectos B +( B)= 0.

8 8 Review of Vectos 6 m Change in a Quantit: The Geek Lette Δ Fequentl we will want to calculate the change in a quantit. Fo eample, we ma want to know the change in a moving object s position o the change in its velocit duing some time inteval. The Geek lette Δ (capital delta suggesting d fo diffeence ) is used to denote the change in a quantit (eithe a scala o a vecto). We use the subscipt i to denote an initial value of a quantit, and the subscipt f to denote the final value of a quantit. If a vecto i denotes the initial position of an object elative to the oigin (its position at the beginning of a time inteval), and f denotes the final position of the object, then m Figue A.12 Relative position vecto. A = 1 A θ A Sting Figue A.13 A unit vecto whose diection is at a known angle fom the + ais. θ θ Figue A.14 A 3D unit vecto and its angles to the,, and aes. θ Δ = f i Δ means change of o f i (displacement) Δt means change of t ot f t i (time inteval) The smbol Δ (delta) alwas means final minus initial, not initial minus final. Fo eample, when a child s height changes fom 1.1 mto1.2m, the change is Δ =+0.1m, a positive numbe. If ou bank account dopped fom $150 to $130, what was the change in ou balance? Δ(bank account)= 20 dollas. Relative Position Vectos Vecto subtaction is used to calculate elative position vectos, vectos which epesent the position of an object elative to anothe object. In Figue A.12 object 1 is at location 1 and object 2 is at location 2. We want the components of a vecto that points fom object 1 to object 2. This is the vecto obtained b subtaction: 2 elative to 1 = 2 1. Note that the fom is alwas final minus initial in these calculations. Unit Vectos and Angles Suppose a taut sting is at an angle θ to the + ais, and we need a unit vecto in the diection of the sting. Figue A.13 shows a unit vecto  pointing along the sting. What is the component of this unit vecto? Conside the tiangle whose base is A and whose hpotenuse is  =1. Fom the definition of the cosine of an angle we have this: cos θ = adjacent hpotenuse = A 1, so A =cosθ In Figue A.13 the angle θ is shown in the fist quadant (θ less than 90 ), but this woks fo lage angles as well. Fo eample, in Figue?? the angle fom the + ais to a unit vecto ˆB is in the second quadant (θ geate than 90 ) and cos θ is negative, which coesponds to B being negative. What is tue fo is also tue fo and. Figue A.14 shows a 3D unit vecto ˆ and indicates the angles between the unit vecto and the,, and aes. Evidentl we can wite Vecto in plane ˆ = cos θ, cos θ, cos θ θ = 90º θ θ Figue A.15 If a vecto lies in the plane, cos θ =sinθ. These thee cosines of the angles between a vecto (o unit vecto) and the coodinate aes ae called the diection cosines of the vecto. The cosine function is neve geate than 1, just as no component of a unit vecto can be geate than 1. A common special case is that of a unit vecto ling in the plane, with eo component (Figue A.15). In this case θ + θ =90, so that cos θ = cos(90 θ )=sinθ, so that ou can epess the cosine of θ as the sine of θ,

9 A.1. DESCRIBING THE 3D WORLD: VECTORS 9 which is often convenient. Howeve, in the geneal 3D case shown in Figue A.14 thee is no such simple elationship among the diection angles, no among thei cosines. FINDING A UNIT VECTOR FROM ANGLES To find a unit vecto if angles ae given: Redaw the vecto of inteest with its tail at the oigin, and detemine the angles between this vecto and the aes. Imagine the vecto 1, 0, 0, which lies on the + ais. θ is the angle though which ou would otate the vecto 1, 0, 0 until its diection matched that of ou vecto. θ is positive, and θ 180. θ is the angle though which ou would otate the vecto 0, 1, 0 until its diection matched that of ou vecto. θ is positive, and θ 180. θ is the angle though which ou would otate the vecto 0, 0, 1 until its diection matched that of ou vecto. θ is positive, and θ 180. EXAMPLE Fom Angle to Unit Vecto A ope ling in the plane, pointing up and to the ight, suppots a climbe at an angle of 20 to the vetical (Figue A.16). What is the unit vecto pointing up along the ope? 20 Figue A.16 A climbe suppoted b a ope. Solution Follow the pocedue given above fo finding a unit vecto fom angles. In Figue A.17 we edaw the vecto with its tail at the oigin, and we detemine the angles between the vecto and the aes. If we otate the unit vecto 1, 0, 0 fom along the + ais to the vecto of inteest, we see that we have to otate though an angle θ =70. To otate the unit vecto 0, 1, 0 fom along the + ais to the vecto of inteest, we have to otate though an angle of θ =20. The angle fom the + ais to ou vecto is θ =90. Theefoe the unit vecto that points along the ope is this: θ = 90º θ = 20º θ = 70º cos 70, cos 20, cos 90 = 0.342, 0.940, 0 Figue A.17 Redaw the vecto with its tail at the oigin. Identif the angles between the positive aes and the vecto. In this eample the vecto lies in the plane. FURTHER DISCUSSION You ma have noticed that the component of the unit vecto can also be calculated as sin 70 =0.940, and it is often useful to ecognie that a vecto component can be obtained using sine instead of cosine. Thee is howeve some advantage alwas to calculate in tems of diection cosines. This is a method that alwas woks, including in 3D, and which avoids having to decide whethe to use a sine o a cosine. Just use the cosine of the angle fom the elevant positive ais to the vecto. EXAMPLE Fom Unit Vecto to Angles A vecto points fom the oigin to the location 600, 0, 300 m. What is the angle that this vecto makes to the ais? To the ais? To the ais?

10 10 Review of Vectos Solution 600, 0, 300 ˆ = = 0.894, 0, ( 600)2 +(0) 2 + (300) 2 m But we also know that ˆ = cos θ, cos θ, cos θ, so cos θ = 0.894, and the accosine gives θ = Similal, cos θ =0, θ =90 (which checks; no component) cos θ =0.447,θ =63.4 θ = 63.4º θ = 153.4º Figue A.18 Look down on the plane. The diffeence in the two angles is 90, as it should be. FURTHER DISCUSSION Looking down on the plane in Figue A.18, ou can see that the diffeence between θ = and θ =63.4 is 90, as it should be. A.2 VECTOR MULTIPLICATION Vectos can be added and subtacted, and the can be multiplied b a scala. Two vectos can also be multiplied, but two diffeent kinds of vecto multiplication ae defined: the dot poduct and the coss poduct. In the pevious volume the dot poduct was intoduced in the contet of wok, and the coss poduct was intoduced in the contet of angula momentum. The Dot Poduct The dot poduct is an opeation involving two vectos. This is encounteed in the epession fo wok in Chapte 6: W = F Δ =(F Δ + F Δ + F Δ) If F = 3, 2, 4 N and Δ = 2, 0, 5 m, then F Δ = ((3 2) + ( 2 0) + (4 5)) N m = 14 N m The esult of a dot poduct opeation is a scala (like the quantit wok). Note that the dot poduct of a vecto with itself gives the squae of the magnitude of the vecto:,,,, =( 2,2,2 )= 2 The magnitude of the dot poduct can also be calculated as: F Δ = F Δ cos θ = F Δ = F Δ whee θ is the angle between the two vectos, placed tail to tail. In the VPthon pogamming language, dot(vecto1,vecto2) gives the dot poduct of two vectos. The Coss Poduct k The coss poduct is discussed in detail in Chapte 18 in the contet of the Biot- Savat law fo finding the magnetic field of moving chages. In the VPthon pogamming language, coss(vecto1,vecto2) gives the coss poduct of two vectos. It is possible to evaluate the coss poduct in tems of unit vectos along the thee aes (Figue A.19). Fist, note that î î=0, ĵ ĵ=0, and ˆk ˆk =0, since when we coss a vecto with itself the angle between the two vectos is eo, and sin 0 =0. Second, î ĵ = ˆk, since the angle is 90 and the ight-hand ule gives a esult in the + diection (out of the page; Figue A.19). On the othe hand, ĵ î= ˆk, because the ight-hand ule gives a esult in the diection (into the Figue A.19 Coss poducts of unit vectos.

11 A.3. SUMMARY 11 page). Similal, ĵ ˆk =î, ˆk ĵ= î, ˆk î=ĵ, and î ˆk = ĵ. Putting this all togethe, we obtain the following geneal esult: A B =(A B A B )î+(a B A B )ĵ+(a B A B )ˆk o A B = (A B A B ), (A B A B ), (A B A B ) This appoach to calculating a coss poduct is paticulal useful in compute calculations. Note the cclic natue of the subscipts:,,. Common Eos in Vecto Multiplication (1) A dot poduct of two vectos esults in a scala, not anothe vecto. (2) A coss poduct of two vectos esults in anothe vecto, not a scala. Technicall, although a component of a vecto is a single numbe, it is not a scala. If ou otate ou coodinate aes, the,, and components of a vecto change, but a tue scala such as m =5kg doesn t change. A.3 SUMMARY Vectos A3Dvecto is a quantit with magnitude and a diection, which can be epessed as a tiple,,. A vecto is indicated b an aow:. A scala is a single numbe. Legal mathematical opeations involving vectos include: adding one vecto to anothe vecto subtacting one vecto fom anothe vecto multipling o dividing a vecto b a scala finding the magnitude of a vecto taking the deivative of a vecto Opeations that ae not legal with vectos include: A vecto cannot be added to a scala A vecto cannot be set equal to a scala A vecto cannot appea in the denominato (ou can t divide b a vecto) The smbol Δ denotes subtaction The smbol Δ (delta) means change of : Δt=t f t i, Δ = f i. Δ alwas means final minus initial.

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review Vecto Calculus: Ae you eady? Vectos in D and 3D Space: Review Pupose: Make cetain that you can define, and use in context, vecto tems, concepts and fomulas listed below: Section 7.-7. find the vecto defined

More information

UNIT CIRCLE TRIGONOMETRY

UNIT CIRCLE TRIGONOMETRY UNIT CIRCLE TRIGONOMETRY The Unit Cicle is the cicle centeed at the oigin with adius unit (hence, the unit cicle. The equation of this cicle is + =. A diagam of the unit cicle is shown below: + = - - -

More information

Coordinate Systems L. M. Kalnins, March 2009

Coordinate Systems L. M. Kalnins, March 2009 Coodinate Sstems L. M. Kalnins, Mach 2009 Pupose of a Coodinate Sstem The pupose of a coodinate sstem is to uniquel detemine the position of an object o data point in space. B space we ma liteall mean

More information

Displacement, Velocity And Acceleration

Displacement, Velocity And Acceleration Displacement, Velocity And Acceleation Vectos and Scalas Position Vectos Displacement Speed and Velocity Acceleation Complete Motion Diagams Outline Scala vs. Vecto Scalas vs. vectos Scala : a eal numbe,

More information

Mechanics 1: Work, Power and Kinetic Energy

Mechanics 1: Work, Power and Kinetic Energy Mechanics 1: Wok, Powe and Kinetic Eneg We fist intoduce the ideas of wok and powe. The notion of wok can be viewed as the bidge between Newton s second law, and eneg (which we have et to define and discuss).

More information

2. TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES

2. TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES . TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES In ode to etend the definitions of the si tigonometic functions to geneal angles, we shall make use of the following ideas: In a Catesian coodinate sstem, an

More information

Skills Needed for Success in Calculus 1

Skills Needed for Success in Calculus 1 Skills Needed fo Success in Calculus Thee is much appehension fom students taking Calculus. It seems that fo man people, "Calculus" is snonmous with "difficult." Howeve, an teache of Calculus will tell

More information

Mechanics 1: Motion in a Central Force Field

Mechanics 1: Motion in a Central Force Field Mechanics : Motion in a Cental Foce Field We now stud the popeties of a paticle of (constant) ass oving in a paticula tpe of foce field, a cental foce field. Cental foces ae ve ipotant in phsics and engineeing.

More information

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses, 3.4. KEPLER S LAWS 145 3.4 Keple s laws You ae familia with the idea that one can solve some mechanics poblems using only consevation of enegy and (linea) momentum. Thus, some of what we see as objects

More information

Moment and couple. In 3-D, because the determination of the distance can be tedious, a vector approach becomes advantageous. r r

Moment and couple. In 3-D, because the determination of the distance can be tedious, a vector approach becomes advantageous. r r Moment and couple In 3-D, because the detemination of the distance can be tedious, a vecto appoach becomes advantageous. o k j i M k j i M o ) ( ) ( ) ( + + M o M + + + + M M + O A Moment about an abita

More information

4.1 - Trigonometric Functions of Acute Angles

4.1 - Trigonometric Functions of Acute Angles 4.1 - Tigonometic Functions of cute ngles a is a half-line that begins at a point and etends indefinitel in some diection. Two as that shae a common endpoint (o vete) fom an angle. If we designate one

More information

Physics 235 Chapter 5. Chapter 5 Gravitation

Physics 235 Chapter 5. Chapter 5 Gravitation Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus

More information

Forces & Magnetic Dipoles. r r τ = μ B r

Forces & Magnetic Dipoles. r r τ = μ B r Foces & Magnetic Dipoles x θ F θ F. = AI τ = U = Fist electic moto invented by Faaday, 1821 Wie with cuent flow (in cup of Hg) otates aound a a magnet Faaday s moto Wie with cuent otates aound a Pemanent

More information

Magnetic Field and Magnetic Forces. Young and Freedman Chapter 27

Magnetic Field and Magnetic Forces. Young and Freedman Chapter 27 Magnetic Field and Magnetic Foces Young and Feedman Chapte 27 Intoduction Reiew - electic fields 1) A chage (o collection of chages) poduces an electic field in the space aound it. 2) The electic field

More information

Episode 401: Newton s law of universal gravitation

Episode 401: Newton s law of universal gravitation Episode 401: Newton s law of univesal gavitation This episode intoduces Newton s law of univesal gavitation fo point masses, and fo spheical masses, and gets students pactising calculations of the foce

More information

Voltage ( = Electric Potential )

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

More information

12. Rolling, Torque, and Angular Momentum

12. Rolling, Torque, and Angular Momentum 12. olling, Toque, and Angula Momentum 1 olling Motion: A motion that is a combination of otational and tanslational motion, e.g. a wheel olling down the oad. Will only conside olling with out slipping.

More information

Semipartial (Part) and Partial Correlation

Semipartial (Part) and Partial Correlation Semipatial (Pat) and Patial Coelation his discussion boows heavily fom Applied Multiple egession/coelation Analysis fo the Behavioal Sciences, by Jacob and Paticia Cohen (975 edition; thee is also an updated

More information

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges The foce between electic chages Coulomb s Law Two chaged objects, of chage q and Q, sepaated by a distance, exet a foce on one anothe. The magnitude of this foce is given by: kqq Coulomb s Law: F whee

More information

Chapter 3 Savings, Present Value and Ricardian Equivalence

Chapter 3 Savings, Present Value and Ricardian Equivalence Chapte 3 Savings, Pesent Value and Ricadian Equivalence Chapte Oveview In the pevious chapte we studied the decision of households to supply hous to the labo maket. This decision was a static decision,

More information

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2 Chapte 5 Example The helium atom has 2 electonic enegy levels: E 3p = 23.1 ev and E 2s = 20.6 ev whee the gound state is E = 0. If an electon makes a tansition fom 3p to 2s, what is the wavelength of the

More information

4a 4ab b 4 2 4 2 5 5 16 40 25. 5.6 10 6 (count number of places from first non-zero digit to

4a 4ab b 4 2 4 2 5 5 16 40 25. 5.6 10 6 (count number of places from first non-zero digit to . Simplify: 0 4 ( 8) 0 64 ( 8) 0 ( 8) = (Ode of opeations fom left to ight: Paenthesis, Exponents, Multiplication, Division, Addition Subtaction). Simplify: (a 4) + (a ) (a+) = a 4 + a 0 a = a 7. Evaluate

More information

An Introduction to Omega

An Introduction to Omega An Intoduction to Omega Con Keating and William F. Shadwick These distibutions have the same mean and vaiance. Ae you indiffeent to thei isk-ewad chaacteistics? The Finance Development Cente 2002 1 Fom

More information

NURBS Drawing Week 5, Lecture 10

NURBS Drawing Week 5, Lecture 10 CS 43/585 Compute Gaphics I NURBS Dawing Week 5, Lectue 1 David Been, William Regli and Maim Pesakhov Geometic and Intelligent Computing Laboato Depatment of Compute Science Deel Univesit http://gicl.cs.deel.edu

More information

Chapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6

Chapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6 Chapte 9 lectic Chages, Foces, an Fiels 6 9. One in a million (0 ) ogen molecules in a containe has lost an electon. We assume that the lost electons have been emove fom the gas altogethe. Fin the numbe

More information

Figure 2. So it is very likely that the Babylonians attributed 60 units to each side of the hexagon. Its resulting perimeter would then be 360!

Figure 2. So it is very likely that the Babylonians attributed 60 units to each side of the hexagon. Its resulting perimeter would then be 360! 1. What ae angles? Last time, we looked at how the Geeks intepeted measument of lengths. Howeve, as fascinated as they wee with geomety, thee was a shape that was much moe enticing than any othe : the

More information

Voltage ( = Electric Potential )

Voltage ( = Electric Potential ) V-1 of 9 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage

More information

Continuous Compounding and Annualization

Continuous Compounding and Annualization Continuous Compounding and Annualization Philip A. Viton Januay 11, 2006 Contents 1 Intoduction 1 2 Continuous Compounding 2 3 Pesent Value with Continuous Compounding 4 4 Annualization 5 5 A Special Poblem

More information

PY1052 Problem Set 8 Autumn 2004 Solutions

PY1052 Problem Set 8 Autumn 2004 Solutions PY052 Poblem Set 8 Autumn 2004 Solutions H h () A solid ball stats fom est at the uppe end of the tack shown and olls without slipping until it olls off the ight-hand end. If H 6.0 m and h 2.0 m, what

More information

The LCOE is defined as the energy price ($ per unit of energy output) for which the Net Present Value of the investment is zero.

The LCOE is defined as the energy price ($ per unit of energy output) for which the Net Present Value of the investment is zero. Poject Decision Metics: Levelized Cost of Enegy (LCOE) Let s etun to ou wind powe and natual gas powe plant example fom ealie in this lesson. Suppose that both powe plants wee selling electicity into the

More information

FXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it.

FXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it. Candidates should be able to : Descibe how a mass ceates a gavitational field in the space aound it. Define gavitational field stength as foce pe unit mass. Define and use the peiod of an object descibing

More information

Spirotechnics! September 7, 2011. Amanda Zeringue, Michael Spannuth and Amanda Zeringue Dierential Geometry Project

Spirotechnics! September 7, 2011. Amanda Zeringue, Michael Spannuth and Amanda Zeringue Dierential Geometry Project Spiotechnics! Septembe 7, 2011 Amanda Zeingue, Michael Spannuth and Amanda Zeingue Dieential Geomety Poject 1 The Beginning The geneal consensus of ou goup began with one thought: Spiogaphs ae awesome.

More information

Financing Terms in the EOQ Model

Financing Terms in the EOQ Model Financing Tems in the EOQ Model Habone W. Stuat, J. Columbia Business School New Yok, NY 1007 hws7@columbia.edu August 6, 004 1 Intoduction This note discusses two tems that ae often omitted fom the standad

More information

Gravitation. AP Physics C

Gravitation. AP Physics C Gavitation AP Physics C Newton s Law of Gavitation What causes YOU to be pulled down? THE EARTH.o moe specifically the EARTH S MASS. Anything that has MASS has a gavitational pull towads it. F α Mm g What

More information

Lesson 8 Ampère s Law and Differential Operators

Lesson 8 Ampère s Law and Differential Operators Lesson 8 Ampèe s Law and Diffeential Opeatos Lawence Rees 7 You ma make a single cop of this document fo pesonal use without witten pemission 8 Intoduction Thee ae significant diffeences between the electic

More information

Chapter 30: Magnetic Fields Due to Currents

Chapter 30: Magnetic Fields Due to Currents d Chapte 3: Magnetic Field Due to Cuent A moving electic chage ceate a magnetic field. One of the moe pactical way of geneating a lage magnetic field (.1-1 T) i to ue a lage cuent flowing though a wie.

More information

Quantity Formula Meaning of variables. 5 C 1 32 F 5 degrees Fahrenheit, 1 bh A 5 area, b 5 base, h 5 height. P 5 2l 1 2w

Quantity Formula Meaning of variables. 5 C 1 32 F 5 degrees Fahrenheit, 1 bh A 5 area, b 5 base, h 5 height. P 5 2l 1 2w 1.4 Rewite Fomulas and Equations Befoe You solved equations. Now You will ewite and evaluate fomulas and equations. Why? So you can apply geometic fomulas, as in Ex. 36. Key Vocabulay fomula solve fo a

More information

The Role of Gravity in Orbital Motion

The Role of Gravity in Orbital Motion ! The Role of Gavity in Obital Motion Pat of: Inquiy Science with Datmouth Developed by: Chistophe Caoll, Depatment of Physics & Astonomy, Datmouth College Adapted fom: How Gavity Affects Obits (Ohio State

More information

Carter-Penrose diagrams and black holes

Carter-Penrose diagrams and black holes Cate-Penose diagams and black holes Ewa Felinska The basic intoduction to the method of building Penose diagams has been pesented, stating with obtaining a Penose diagam fom Minkowski space. An example

More information

AP Physics Electromagnetic Wrap Up

AP Physics Electromagnetic Wrap Up AP Physics Electomagnetic Wap Up Hee ae the gloious equations fo this wondeful section. F qsin This is the equation fo the magnetic foce acting on a moing chaged paticle in a magnetic field. The angle

More information

Exam 3: Equation Summary

Exam 3: Equation Summary MASSACHUSETTS INSTITUTE OF TECHNOLOGY Depatment of Physics Physics 8.1 TEAL Fall Tem 4 Momentum: p = mv, F t = p, Fext ave t= t f t= Exam 3: Equation Summay total = Impulse: I F( t ) = p Toque: τ = S S,P

More information

Chapter 17 The Kepler Problem: Planetary Mechanics and the Bohr Atom

Chapter 17 The Kepler Problem: Planetary Mechanics and the Bohr Atom Chapte 7 The Keple Poblem: Planetay Mechanics and the Boh Atom Keple s Laws: Each planet moves in an ellipse with the sun at one focus. The adius vecto fom the sun to a planet sweeps out equal aeas in

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere.

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere. Chapte.3 What is the magnitude of a point chage whose electic field 5 cm away has the magnitude of.n/c. E E 5.56 1 11 C.5 An atom of plutonium-39 has a nuclea adius of 6.64 fm and atomic numbe Z94. Assuming

More information

Lab #7: Energy Conservation

Lab #7: Energy Conservation Lab #7: Enegy Consevation Photo by Kallin http://www.bungeezone.com/pics/kallin.shtml Reading Assignment: Chapte 7 Sections 1,, 3, 5, 6 Chapte 8 Sections 1-4 Intoduction: Pehaps one of the most unusual

More information

Multiple choice questions [60 points]

Multiple choice questions [60 points] 1 Multiple choice questions [60 points] Answe all o the ollowing questions. Read each question caeully. Fill the coect bubble on you scanton sheet. Each question has exactly one coect answe. All questions

More information

Experiment 6: Centripetal Force

Experiment 6: Centripetal Force Name Section Date Intoduction Expeiment 6: Centipetal oce This expeiment is concened with the foce necessay to keep an object moving in a constant cicula path. Accoding to Newton s fist law of motion thee

More information

Deflection of Electrons by Electric and Magnetic Fields

Deflection of Electrons by Electric and Magnetic Fields Physics 233 Expeiment 42 Deflection of Electons by Electic and Magnetic Fields Refeences Loain, P. and D.R. Coson, Electomagnetism, Pinciples and Applications, 2nd ed., W.H. Feeman, 199. Intoduction An

More information

Graphs of Equations. A coordinate system is a way to graphically show the relationship between 2 quantities.

Graphs of Equations. A coordinate system is a way to graphically show the relationship between 2 quantities. Gaphs of Equations CHAT Pe-Calculus A coodinate sstem is a wa to gaphicall show the elationship between quantities. Definition: A solution of an equation in two vaiables and is an odeed pai (a, b) such

More information

Math, Trigonometry and Vectors. Geometry. Trig Definitions. sin(θ) = opp hyp. cos(θ) = adj hyp. tan(θ) = opp adj. Here's a familiar image.

Math, Trigonometry and Vectors. Geometry. Trig Definitions. sin(θ) = opp hyp. cos(θ) = adj hyp. tan(θ) = opp adj. Here's a familiar image. Math, Trigonometr and Vectors Geometr Trig Definitions Here's a familiar image. To make predictive models of the phsical world, we'll need to make visualizations, which we can then turn into analtical

More information

Multiple choice questions [70 points]

Multiple choice questions [70 points] Multiple choice questions [70 points] Answe all of the following questions. Read each question caefull. Fill the coect bubble on ou scanton sheet. Each question has exactl one coect answe. All questions

More information

STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION

STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION Page 1 STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION C. Alan Blaylock, Hendeson State Univesity ABSTRACT This pape pesents an intuitive appoach to deiving annuity fomulas fo classoom use and attempts

More information

sin(θ) = opp hyp cos(θ) = adj hyp tan(θ) = opp adj

sin(θ) = opp hyp cos(θ) = adj hyp tan(θ) = opp adj Math, Trigonometr and Vectors Geometr 33º What is the angle equal to? a) α = 7 b) α = 57 c) α = 33 d) α = 90 e) α cannot be determined α Trig Definitions Here's a familiar image. To make predictive models

More information

est using the formula I = Prt, where I is the interest earned, P is the principal, r is the interest rate, and t is the time in years.

est using the formula I = Prt, where I is the interest earned, P is the principal, r is the interest rate, and t is the time in years. 9.2 Inteest Objectives 1. Undestand the simple inteest fomula. 2. Use the compound inteest fomula to find futue value. 3. Solve the compound inteest fomula fo diffeent unknowns, such as the pesent value,

More information

Section V.2: Magnitudes, Directions, and Components of Vectors

Section V.2: Magnitudes, Directions, and Components of Vectors Section V.: Magnitudes, Directions, and Components of Vectors Vectors in the plane If we graph a vector in the coordinate plane instead of just a grid, there are a few things to note. Firstl, directions

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this inestigation

More information

Questions & Answers Chapter 10 Software Reliability Prediction, Allocation and Demonstration Testing

Questions & Answers Chapter 10 Software Reliability Prediction, Allocation and Demonstration Testing M13914 Questions & Answes Chapte 10 Softwae Reliability Pediction, Allocation and Demonstation Testing 1. Homewok: How to deive the fomula of failue ate estimate. λ = χ α,+ t When the failue times follow

More information

Fluids Lecture 15 Notes

Fluids Lecture 15 Notes Fluids Lectue 15 Notes 1. Unifom flow, Souces, Sinks, Doublets Reading: Andeson 3.9 3.12 Unifom Flow Definition A unifom flow consists of a velocit field whee V = uî + vĵ is a constant. In 2-D, this velocit

More information

Lesson 7 Gauss s Law and Electric Fields

Lesson 7 Gauss s Law and Electric Fields Lesson 7 Gauss s Law and Electic Fields Lawence B. Rees 7. You may make a single copy of this document fo pesonal use without witten pemission. 7. Intoduction While it is impotant to gain a solid conceptual

More information

CHAPTER 10 Aggregate Demand I

CHAPTER 10 Aggregate Demand I CHAPTR 10 Aggegate Demand I Questions fo Review 1. The Keynesian coss tells us that fiscal policy has a multiplied effect on income. The eason is that accoding to the consumption function, highe income

More information

Model Question Paper Mathematics Class XII

Model Question Paper Mathematics Class XII Model Question Pape Mathematics Class XII Time Allowed : 3 hous Maks: 100 Ma: Geneal Instuctions (i) The question pape consists of thee pats A, B and C. Each question of each pat is compulsoy. (ii) Pat

More information

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C Geneal Physics - PH Winte 6 Bjoen Seipel The Electic Potential, Electic Potential Enegy and Enegy Consevation Electic Potential Enegy U is the enegy of a chaged object in an extenal electic field (Unit

More information

Lecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3

Lecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3 Lectue 16: Colo and Intensity and he made him a coat of many colous. Genesis 37:3 1. Intoduction To display a pictue using Compute Gaphics, we need to compute the colo and intensity of the light at each

More information

Concept and Experiences on using a Wiki-based System for Software-related Seminar Papers

Concept and Experiences on using a Wiki-based System for Software-related Seminar Papers Concept and Expeiences on using a Wiki-based System fo Softwae-elated Semina Papes Dominik Fanke and Stefan Kowalewski RWTH Aachen Univesity, 52074 Aachen, Gemany, {fanke, kowalewski}@embedded.wth-aachen.de,

More information

Converting knowledge Into Practice

Converting knowledge Into Practice Conveting knowledge Into Pactice Boke Nightmae srs Tend Ride By Vladimi Ribakov Ceato of Pips Caie 20 of June 2010 2 0 1 0 C o p y i g h t s V l a d i m i R i b a k o v 1 Disclaime and Risk Wanings Tading

More information

Solution Derivations for Capa #8

Solution Derivations for Capa #8 Solution Deivations fo Capa #8 1) A ass spectoete applies a voltage of 2.00 kv to acceleate a singly chaged ion (+e). A 0.400 T field then bends the ion into a cicula path of adius 0.305. What is the ass

More information

The Binomial Distribution

The Binomial Distribution The Binomial Distibution A. It would be vey tedious if, evey time we had a slightly diffeent poblem, we had to detemine the pobability distibutions fom scatch. Luckily, thee ae enough similaities between

More information

AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM

AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM Main Golub Faculty of Electical Engineeing and Computing, Univesity of Zageb Depatment of Electonics, Micoelectonics,

More information

The Detection of Obstacles Using Features by the Horizon View Camera

The Detection of Obstacles Using Features by the Horizon View Camera The Detection of Obstacles Using Featues b the Hoizon View Camea Aami Iwata, Kunihito Kato, Kazuhiko Yamamoto Depatment of Infomation Science, Facult of Engineeing, Gifu Univesit aa@am.info.gifu-u.ac.jp

More information

Addition and Subtraction of Vectors

Addition and Subtraction of Vectors ddition and Subtraction of Vectors 1 ppendi ddition and Subtraction of Vectors In this appendi the basic elements of vector algebra are eplored. Vectors are treated as geometric entities represented b

More information

Saturated and weakly saturated hypergraphs

Saturated and weakly saturated hypergraphs Satuated and weakly satuated hypegaphs Algebaic Methods in Combinatoics, Lectues 6-7 Satuated hypegaphs Recall the following Definition. A family A P([n]) is said to be an antichain if we neve have A B

More information

Problem Set # 9 Solutions

Problem Set # 9 Solutions Poblem Set # 9 Solutions Chapte 12 #2 a. The invention of the new high-speed chip inceases investment demand, which shifts the cuve out. That is, at evey inteest ate, fims want to invest moe. The incease

More information

Thank you for participating in Teach It First!

Thank you for participating in Teach It First! Thank you fo paticipating in Teach It Fist! This Teach It Fist Kit contains a Common Coe Suppot Coach, Foundational Mathematics teache lesson followed by the coesponding student lesson. We ae confident

More information

CLASS XI CHAPTER 3. Theorem 1 (sine formula) In any triangle, sides are proportional to the sines of the opposite angles. That is, in a triangle ABC

CLASS XI CHAPTER 3. Theorem 1 (sine formula) In any triangle, sides are proportional to the sines of the opposite angles. That is, in a triangle ABC CLASS XI Anneue I CHAPTER.6. Poofs and Simple Applications of sine and cosine fomulae Let ABC be a tiangle. By angle A we mean te angle between te sides AB and AC wic lies between 0 and 80. Te angles B

More information

TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION

TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION MISN-0-34 TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION shaft TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION by Kiby Mogan, Chalotte, Michigan 1. Intoduction..............................................

More information

PAN STABILITY TESTING OF DC CIRCUITS USING VARIATIONAL METHODS XVIII - SPETO - 1995. pod patronatem. Summary

PAN STABILITY TESTING OF DC CIRCUITS USING VARIATIONAL METHODS XVIII - SPETO - 1995. pod patronatem. Summary PCE SEMINIUM Z PODSTW ELEKTOTECHNIKI I TEOII OBWODÓW 8 - TH SEMIN ON FUNDMENTLS OF ELECTOTECHNICS ND CICUIT THEOY ZDENĚK BIOLEK SPŠE OŽNO P.., CZECH EPUBLIC DLIBO BIOLEK MILITY CDEMY, BNO, CZECH EPUBLIC

More information

Physics HSC Course Stage 6. Space. Part 1: Earth s gravitational field

Physics HSC Course Stage 6. Space. Part 1: Earth s gravitational field Physics HSC Couse Stage 6 Space Pat 1: Eath s gavitational field Contents Intoduction... Weight... 4 The value of g... 7 Measuing g...8 Vaiations in g...11 Calculating g and W...13 You weight on othe

More information

The Supply of Loanable Funds: A Comment on the Misconception and Its Implications

The Supply of Loanable Funds: A Comment on the Misconception and Its Implications JOURNL OF ECONOMICS ND FINNCE EDUCTION Volume 7 Numbe 2 Winte 2008 39 The Supply of Loanable Funds: Comment on the Misconception and Its Implications. Wahhab Khandke and mena Khandke* STRCT Recently Fields-Hat

More information

Chris J. Skinner The probability of identification: applying ideas from forensic statistics to disclosure risk assessment

Chris J. Skinner The probability of identification: applying ideas from forensic statistics to disclosure risk assessment Chis J. Skinne The pobability of identification: applying ideas fom foensic statistics to disclosue isk assessment Aticle (Accepted vesion) (Refeeed) Oiginal citation: Skinne, Chis J. (2007) The pobability

More information

Questions for Review. By buying bonds This period you save s, next period you get s(1+r)

Questions for Review. By buying bonds This period you save s, next period you get s(1+r) MACROECONOMICS 2006 Week 5 Semina Questions Questions fo Review 1. How do consumes save in the two-peiod model? By buying bonds This peiod you save s, next peiod you get s() 2. What is the slope of a consume

More information

INVESTIGATION OF FLOW INSIDE AN AXIAL-FLOW PUMP OF GV IMP TYPE

INVESTIGATION OF FLOW INSIDE AN AXIAL-FLOW PUMP OF GV IMP TYPE 1 INVESTIGATION OF FLOW INSIDE AN AXIAL-FLOW PUMP OF GV IMP TYPE ANATOLIY A. YEVTUSHENKO 1, ALEXEY N. KOCHEVSKY 1, NATALYA A. FEDOTOVA 1, ALEXANDER Y. SCHELYAEV 2, VLADIMIR N. KONSHIN 2 1 Depatment of

More information

Software Engineering and Development

Software Engineering and Development I T H E A 67 Softwae Engineeing and Development SOFTWARE DEVELOPMENT PROCESS DYNAMICS MODELING AS STATE MACHINE Leonid Lyubchyk, Vasyl Soloshchuk Abstact: Softwae development pocess modeling is gaining

More information

Week 3-4: Permutations and Combinations

Week 3-4: Permutations and Combinations Week 3-4: Pemutations and Combinations Febuay 24, 2016 1 Two Counting Pinciples Addition Pinciple Let S 1, S 2,, S m be disjoint subsets of a finite set S If S S 1 S 2 S m, then S S 1 + S 2 + + S m Multiplication

More information

INITIAL MARGIN CALCULATION ON DERIVATIVE MARKETS OPTION VALUATION FORMULAS

INITIAL MARGIN CALCULATION ON DERIVATIVE MARKETS OPTION VALUATION FORMULAS INITIAL MARGIN CALCULATION ON DERIVATIVE MARKETS OPTION VALUATION FORMULAS Vesion:.0 Date: June 0 Disclaime This document is solely intended as infomation fo cleaing membes and othes who ae inteested in

More information

Definitions and terminology

Definitions and terminology I love the Case & Fai textbook but it is out of date with how monetay policy woks today. Please use this handout to supplement the chapte on monetay policy. The textbook assumes that the Fedeal Reseve

More information

Left- and Right-Brain Preferences Profile

Left- and Right-Brain Preferences Profile Left- and Right-Bain Pefeences Pofile God gave man a total bain, and He expects us to pesent both sides of ou bains back to Him so that He can use them unde the diection of His Holy Spiit as He so desies

More information

Symmetric polynomials and partitions Eugene Mukhin

Symmetric polynomials and partitions Eugene Mukhin Symmetic polynomials and patitions Eugene Mukhin. Symmetic polynomials.. Definition. We will conside polynomials in n vaiables x,..., x n and use the shotcut p(x) instead of p(x,..., x n ). A pemutation

More information

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of Homewok VI Ch. 7 - Poblems 15, 19, 22, 25, 35, 43, 51. Poblem 15 (a) The centipetal acceleation of a point on the equato of the Eath is given by v2. The velocity of the eath can be found by taking the

More information

Summary: Vectors. This theorem is used to find any points (or position vectors) on a given line (direction vector). Two ways RT can be applied:

Summary: Vectors. This theorem is used to find any points (or position vectors) on a given line (direction vector). Two ways RT can be applied: Summ: Vectos ) Rtio Theoem (RT) This theoem is used to find n points (o position vectos) on given line (diection vecto). Two ws RT cn e pplied: Cse : If the point lies BETWEEN two known position vectos

More information

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013 PHYSICS 111 HOMEWORK SOLUTION #13 May 1, 2013 0.1 In intoductoy physics laboatoies, a typical Cavendish balance fo measuing the gavitational constant G uses lead sphees with masses of 2.10 kg and 21.0

More information

ON THE (Q, R) POLICY IN PRODUCTION-INVENTORY SYSTEMS

ON THE (Q, R) POLICY IN PRODUCTION-INVENTORY SYSTEMS ON THE R POLICY IN PRODUCTION-INVENTORY SYSTEMS Saifallah Benjaafa and Joon-Seok Kim Depatment of Mechanical Engineeing Univesity of Minnesota Minneapolis MN 55455 Abstact We conside a poduction-inventoy

More information

Charges, Coulomb s Law, and Electric Fields

Charges, Coulomb s Law, and Electric Fields Q&E -1 Chages, Coulomb s Law, and Electic ields Some expeimental facts: Expeimental fact 1: Electic chage comes in two types, which we call (+) and ( ). An atom consists of a heavy (+) chaged nucleus suounded

More information

CHAPTER 9 THE TWO BODY PROBLEM IN TWO DIMENSIONS

CHAPTER 9 THE TWO BODY PROBLEM IN TWO DIMENSIONS 9. Intoduction CHAPTER 9 THE TWO BODY PROBLEM IN TWO DIMENSIONS In this chapte we show how Keple s laws can be deived fom Newton s laws of motion and gavitation, and consevation of angula momentum, and

More information

Chapter 4: Matrix Norms

Chapter 4: Matrix Norms EE448/58 Vesion.0 John Stensby Chate 4: Matix Noms The analysis of matix-based algoithms often equies use of matix noms. These algoithms need a way to quantify the "size" of a matix o the "distance" between

More information

Chapter 4: Fluid Kinematics

Chapter 4: Fluid Kinematics Oveview Fluid kinematics deals with the motion of fluids without consideing the foces and moments which ceate the motion. Items discussed in this Chapte. Mateial deivative and its elationship to Lagangian

More information

Gravitation and Kepler s Laws Newton s Law of Universal Gravitation in vectorial. Gm 1 m 2. r 2

Gravitation and Kepler s Laws Newton s Law of Universal Gravitation in vectorial. Gm 1 m 2. r 2 F Gm Gavitation and Keple s Laws Newton s Law of Univesal Gavitation in vectoial fom: F 12 21 Gm 1 m 2 12 2 ˆ 12 whee the hat (ˆ) denotes a unit vecto as usual. Gavity obeys the supeposition pinciple,

More information

Chapter 2. Electrostatics

Chapter 2. Electrostatics Chapte. Electostatics.. The Electostatic Field To calculate the foce exeted by some electic chages,,, 3,... (the souce chages) on anothe chage Q (the test chage) we can use the pinciple of supeposition.

More information

Experiment MF Magnetic Force

Experiment MF Magnetic Force Expeiment MF Magnetic Foce Intoduction The magnetic foce on a cuent-caying conducto is basic to evey electic moto -- tuning the hands of electic watches and clocks, tanspoting tape in Walkmans, stating

More information

Lab M4: The Torsional Pendulum and Moment of Inertia

Lab M4: The Torsional Pendulum and Moment of Inertia M4.1 Lab M4: The Tosional Pendulum and Moment of netia ntoduction A tosional pendulum, o tosional oscillato, consists of a disk-like mass suspended fom a thin od o wie. When the mass is twisted about the

More information

Risk Sensitive Portfolio Management With Cox-Ingersoll-Ross Interest Rates: the HJB Equation

Risk Sensitive Portfolio Management With Cox-Ingersoll-Ross Interest Rates: the HJB Equation Risk Sensitive Potfolio Management With Cox-Ingesoll-Ross Inteest Rates: the HJB Equation Tomasz R. Bielecki Depatment of Mathematics, The Notheasten Illinois Univesity 55 Noth St. Louis Avenue, Chicago,

More information