Rectangular Polar Parametric

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Rectangular Polar Parametric"

Transcript

1 Hrold s AP Clculus BC Rectngulr Polr Prmetric Chet Sheet 15 Octoer 2017 Point Line Rectngulr Polr Prmetric f(x) = y (x, y) (, ) Slope-Intercept Form: y = mx + Point-Slope Form: y y 0 = m (x x 0 ) Generl Form: Ax + By + C = 0 Clculus Form: f(x) = f () x + f(0) (r, θ) or r θ Polr Rect. Rect. Polr x = r cos θ y = r sin θ tn θ = y x r 2 = x 2 + y 2 r = ± x 2 + y 2 θ = tn 1 ( y x ) Point (,) in Rectngulr: x(t) = y(t) = <, > t = 3 rd vrile, usully time, with 1 degree of freedom (df) < x, y > = < x 0, y 0 > + t <, > < x, y > = < x 0 + t, y 0 + t > where <, > = < x 2 x 1, y 2 y 1 > x(t) = x 0 + t y(t) = y 0 + t m = y x = y 2 y 1 x 2 x 1 = r = r 0 + sv + tw Plne n x (x x 0 ) +n y (y y 0 ) + n z (z z 0 ) = 0 Vector Form: n (r r 0 ) = 0 where: v nd w re given vectors defining the plne r 0 is the vector of fixed point on the plne Copyright y Hrold Toomey, WyzAnt Tutor 1

2 Rectngulr Polr Prmetric. Generl Eqution for All Conics: Generl Eqution for All Conics: Conics Ax 2 + Bxy + Cy 2 + Dx + Ey + F = 0 where Line: A = B = C = 0 Circle: A = C nd B = 0 Ellipse: AC > 0 or B 2 4AC < 0 Prol: AC = 0 or B 2 4AC = 0 Hyperol: AC < 0 or B 2 4AC > 0 Note: If A + C = 0, squre hyperol Rottion: If B 0, then rotte coordinte system: A C cot 2θ = B x = x cos θ y sin θ y = y cos θ + x sin θ New = (x, y ), Old = (x, y) rottes through ngle θ from x-xis r = p 1 e cos θ (1 e 2 ) 0 e < 1 where p = { 2d for { e = 1 (e 2 1) e > 1 p = semi-ltus rectum or the line segment running from the focus to the curve in direction prllel to the directrix Eccentricity: Circle e = 0 Ellipse 0 e < 1 Prol e = 1 Hyperol e > 1 Copyright y Hrold Toomey, WyzAnt Tutor 2

3 Rectngulr Polr Prmetric. x 2 + y 2 = r 2 (x h) 2 + (y k) 2 = r 2 Centered t Origin: r = (constnt) θ = θ [0, 2π] or [0, 360 ] Circle Center: (h, k) Vertices: NA Focus: (h, k) Centered t (r 0, φ): r 2 + r 0 2 2rr 0 cos(θ φ) = R 2 Hint: Lw of Cosines or r = r 0 cos(θ φ) + 2 r 0 2 sin 2 (θ φ) x(t) = r cos(t) + h y(t) = r sin(t) + k [t min, t mx ] = [0, 2π) (h, k) = center of circle (h, k) Copyright y Hrold Toomey, WyzAnt Tutor 3

4 Rectngulr Polr Prmetric. (x h) 2 2 (y k)2 + 2 = 1 Center: (h, k) Vertices: (h ±, k) nd (h, k ± ) Foci: (h ± c, k) Focus length, c, from center: c = 2 2 Ellipse: r = (1 e2 ) for 0 e < e cos θ where e = c = 2 2 reltive to center (h,k) x(t) = cos(t) + h y(t) = sin(t) + k [t min, t mx ] = [0, 2π] (h, k) = center of ellipse Rotted Ellipse: x(t) = cos t cos θ sin t sin θ + h y(t) = cos t sin θ + sin t cos θ + k Ellipse θ = the ngle etween the x-xis nd the mjor xis of the ellipse Interesting Note: The sum of the distnces from ech focus to point on the curve is constnt. d 1 + d 2 = k Copyright y Hrold Toomey, WyzAnt Tutor 4

5 Prol Rectngulr Polr Prmetric. Verticl Axis of Symmetry: x 2 = 4 py (x h) 2 = 4p(y k) Vertex: (h, k) Focus: (h, k + p) Directrix: y = k p Horizontl Axis of Symmetry: y 2 = 4 px (y k) 2 = 4p(x h) Vertex: (h, k) Focus: (h + p, k) Directrix: x = h p Prol: 2d r = for e = e cos θ where d = 2p Trigonometric Form: y = x 2 r sin θ = r 2 cos 2 θ sin θ r = cos 2 = tn θ sec θ θ Verticl Axis of Symmetry: x(t) = 2pt + h y(t) = pt 2 + k (opens upwrds) or y(t) = pt 2 k (opens downwrds) [t min, t mx ] = [ c, c] (h, k) = vertex of prol Horizontl Axis of Symmetry: y(t) = 2pt + k x(t) = pt 2 + h (opens to the right) or x(t) = pt 2 h (opens to the left) [t min, t mx ] = [ c, c] (h, k) = vertex of prol Projectile Motion: x(t) = x 0 + v x t y(t) = y 0 + v y t 16t 2 feet y(t) = y 0 + v y t 4.9t 2 meters v x = v cos θ v y = v sin θ Generl Form: x = At 2 + Bt + C y = Dt 2 + Et + F where A nd D hve the sme sign Copyright y Hrold Toomey, WyzAnt Tutor 5

6 Hyperol Rectngulr Polr Prmetric. (x h) 2 2 (y k)2 2 = 1 Center: (h, k) Vertices: (h ±, k) Foci: (h ± c, k) Focus length, c, from center: c = Hyperol: r = (e2 1) for e > e cos θ Eccentricity: where e = c = = sec θ > 1 reltive to center (h,k) Left-Right Opening Hyperol: x(t) = sec( t) + h y(t) = tn( t) + k [t min, t mx ] = [ c, c] (h, k) = vertex of hyperol Up-Down Opening Hyperol: x(t) = tn(t) + h y(t) = sec(t) + k [t min, t mx ] = [ c, c] (h, k) = vertex of hyperol p = semi-ltus rectum or the line segment running from the focus to the curve in the directions θ = ± π 2 Interesting Note: The difference etween the distnces from ech focus to point on the curve is constnt. d 1 d 2 = k Generl Form: x(t) = At 2 + Bt + C y(t) = Dt 2 + Et + F where A nd D hve different signs Copyright y Hrold Toomey, WyzAnt Tutor 6

7 Rectngulr Polr Prmetric. 1 st Derivtive 2 nd Derivtive f f(x + h) f(x) (x) = lim h 0 h f f(x) f(c) (c) = lim x c x c f (x) = dy = y = D x f (x) = d (dy ) = d2 y 2 = y dy = dy = dr sin θ + r cos θ dr cos θ r sin θ Hint: Use Product Rule for y = r sin θ x = r cos θ d 2 y 2 = d (dy ) = d (dy ) dy = dy, provided 0 d 2 y 2 = d (dy ) = Riemnn Sum: n d (dy ) S = f(y i )(x i x i 1 ) i 1 Left Sum: S = ( 1 n ) [f() + f ( + 1 n ) + f ( + 2 n ) + + f( 1 n )] Integrl F(x) = f(x) = F() F() Middle Sum: S = ( ) [f ( + ) + f ( + n 2n 2n ) + + f( 1 2n )] Right Sum: S = ( 1 n ) [f ( + 1 n ) + f ( + 2 n ) + + f()] Copyright y Hrold Toomey, WyzAnt Tutor 7

8 Inverse Functions Arc Length Rectngulr Polr Prmetric. f(f 1 (x)) = f 1 (f(x)) = x Inverse Function Theorem: f 1 1 () = f () where = f () L = 1 + [f (x)] 2 Proof: s = (x x 0 ) 2 + (y y 0 ) 2 s = ( x) 2 + ( y) 2 ds = 2 + dy 2 ds = 2 + dy 2 ( 2 2) ds = 2 + ( dy ) 2 2 ds = 2 (1 + ( dy ) 2 ) if y = sin θ if y = cos θ if y = tn θ if y = csc θ if y = sec θ if y = cot θ L = ds ds = r 2 + ( dr ) 2 Circle: L = s = rθ then θ = sin 1 y then θ = cos 1 y then θ = tn 1 y then θ = csc 1 y then θ = sec 1 y then θ = cot 1 y Proof: L = (frction of circumference) π (dimeter) L = ( θ ) π (2r) = rθ 2π θ = rcsin y θ = rccos y θ = rctn y θ = rccsc y θ = rcsec y θ = rccot y L = ( L = ( + ( dy + ( dy + ( dz ds = 1 + ( dy ) 2 L = ds Perimeter Squre: P = 4s Rectngle: P = 2l + 2w Tringle: P = + + c Circle: C = πd = 2πr Ellipse: C π( + ) π Ellipse: C = ( c )2 sin 2 θ 0 Copyright y Hrold Toomey, WyzAnt Tutor 8

9 Are Lterl Surfce Are Rectngulr Polr Prmetric. Squre: A = s² Rectngle: A = lw Rhomus: A = ½ Prllelogrm: A = h Trpezoid: A = ( 1+ 2 ) h 2 Kite: A = d 1 d 2 2 Tringle: A = ½ h Tringle: A = ½ sin(c) Tringle: A = s(s )(s )(s c), where s = ++c 2 Equilterl Tringle: A = ¼ 3s 2 Frustum: A = 1 3 ( 1+ 2 ) h 2 Circle: A = πr² Circulr Sector: A = ½ r²θ Ellipse: A = π Cylinder: S = 2πrh Cone: S = πrl S = 2π f(x) 1 + [f (x)] 2 A = 1 2 [f(θ)]2 where r = f(θ) Proof: Are of sector: A = s dr = r θ dr = 1 2 r2 θ where rc length s = r θ For rottion out the x-xis: S = 2πy ds For rottion out the y-xis: S = 2πx ds A = g(t) f (t) where f(t) = x nd g(t) = y or x(t) = f(t) nd y(t) = g(t) Simplified: A = y(t) (t) Proof: f(x) y = f(x) = g(t) = df(t) = f (t) For rottion out the x-xis: S = 2πy ds For rottion out the y-xis: S = 2πx ds ds = r 2 + ( dr 2 ) r = f(θ), θ ds = ( 2 ) + ( dy 2 ) if x = f(t), y = g(t), t Copyright y Hrold Toomey, WyzAnt Tutor 9

10 Totl Surfce Are Surfce of Revolution Volume Rectngulr Polr Prmetric. Cue: S = 6s² Rectngulr Box: S = 2lw + 2wh + 2hl Regulr Tetrhedron: S = 2h Cylinder: S = 2πr (r + h) Cone: S = πr² + πrl = πr (r + l) For revolution out the x-xis: A = 2π f(x) 1 + ( dy ) 2 For revolution out the y-xis: A = 2π x 1 + ( dy ) 2 dy Cue: V = s³ Rectngulr Prism: V = lwh Cylinder: V = πr²h Tringulr Prism: V= Bh Tetrhedron: V= ⅓ h Pyrmid: V = ⅓ Bh Cone: V = ⅓ h = ⅓ πr²h Sphere: S = 4πr² Ellipsoid: S = (too complex) For revolution out the x-xis: A = 2π r cos θ r 2 + ( dr ) 2 For revolution out the y-xis: A = 2π r sin θ Sphere: V = 4 3 πr3 r 2 + ( dr ) 2 Ellipsoid: V = 4 3 πc For revolution out the x-xis: A = 2π y(t) ( + ( dy For revolution out the y-xis: A = 2π x(t) ( + ( dy Copyright y Hrold Toomey, WyzAnt Tutor 10

11 Rectngulr Polr Prmetric. Disc Method - Rottion out the x- xis: V = π [f(x)] 2 Cylindricl Shell Method: = (re of circle) d(thickness) Disc Method: Volume of Revolution Wsher Method - Rottion out the x-xis: V = π { [f(x)] 2 [g(x)] 2 } Cylinder Method - Rottion out the y-xis: V = 2πx f(x) = (circumference) (hight) Copyright y Hrold Toomey, WyzAnt Tutor 11

Rectangular Polar/Cylindrical Spherical Parametric Vector Matrix

Rectangular Polar/Cylindrical Spherical Parametric Vector Matrix Hrold s Clculus 3 ulti-cordinte System Chet Sheet 15 Octoer 017 Point Rectngulr Polr/Cylindricl Sphericl Prmetric Vector trix -D f(x) y (x, y) (, ) 3-D f(x, y) z (x, y, z) 4-D f(x, y, z) w (x, y, z, w)

Διαβάστε περισσότερα

Rectangular Polar Parametric

Rectangular Polar Parametric Harold s Precalculus Rectangular Polar Parametric Cheat Sheet 15 October 2017 Point Line Rectangular Polar Parametric f(x) = y (x, y) (a, b) Slope-Intercept Form: y = mx + b Point-Slope Form: y y 0 = m

Διαβάστε περισσότερα

CHAPTER (2) Electric Charges, Electric Charge Densities and Electric Field Intensity

CHAPTER (2) Electric Charges, Electric Charge Densities and Electric Field Intensity CHAPTE () Electric Chrges, Electric Chrge Densities nd Electric Field Intensity Chrge Configurtion ) Point Chrge: The concept of the point chrge is used when the dimensions of n electric chrge distriution

Διαβάστε περισσότερα

CBC MATHEMATICS DIVISION MATH 2412-PreCalculus Exam Formula Sheets

CBC MATHEMATICS DIVISION MATH 2412-PreCalculus Exam Formula Sheets System of Equations and Matrices 3 Matrix Row Operations: MATH 41-PreCalculus Switch any two rows. Multiply any row by a nonzero constant. Add any constant-multiple row to another Even and Odd functions

Διαβάστε περισσότερα

Trigonometric Formula Sheet

Trigonometric Formula Sheet Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ

Διαβάστε περισσότερα

Homework 8 Model Solution Section

Homework 8 Model Solution Section MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx

Διαβάστε περισσότερα

Equations. BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1. du dv. FTLI : f (B) f (A) = f dr. F dr = Green s Theorem : y da

Equations. BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1. du dv. FTLI : f (B) f (A) = f dr. F dr = Green s Theorem : y da BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1 Equations r(t) = x(t) î + y(t) ĵ + z(t) k r = r (t) t s = r = r (t) t r(u, v) = x(u, v) î + y(u, v) ĵ + z(u, v) k S = ( ( ) r r u r v = u

Διαβάστε περισσότερα

Chapter 7b, Torsion. τ = 0. τ T. T τ D'' A'' C'' B'' 180 -rotation around axis C'' B'' D'' A'' A'' D'' 180 -rotation upside-down C'' B''

Chapter 7b, Torsion. τ = 0. τ T. T τ D'' A'' C'' B'' 180 -rotation around axis C'' B'' D'' A'' A'' D'' 180 -rotation upside-down C'' B'' Chpter 7b, orsion τ τ τ ' D' B' C' '' B'' B'' D'' C'' 18 -rottion round xis C'' B'' '' D'' C'' '' 18 -rottion upside-down D'' stright lines in the cross section (cross sectionl projection) remin stright

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

Review-2 and Practice problems. sin 2 (x) cos 2 (x)(sin(x)dx) (1 cos 2 (x)) cos 2 (x)(sin(x)dx) let u = cos(x), du = sin(x)dx. = (1 u 2 )u 2 ( du)

Review-2 and Practice problems. sin 2 (x) cos 2 (x)(sin(x)dx) (1 cos 2 (x)) cos 2 (x)(sin(x)dx) let u = cos(x), du = sin(x)dx. = (1 u 2 )u 2 ( du) . Trigonometric Integrls. ( sin m (x cos n (x Cse-: m is odd let u cos(x Exmple: sin 3 (x cos (x Review- nd Prctice problems sin 3 (x cos (x Cse-: n is odd let u sin(x Exmple: cos 5 (x cos 5 (x sin (x

Διαβάστε περισσότερα

If ABC is any oblique triangle with sides a, b, and c, the following equations are valid. 2bc. (a) a 2 b 2 c 2 2bc cos A or cos A b2 c 2 a 2.

If ABC is any oblique triangle with sides a, b, and c, the following equations are valid. 2bc. (a) a 2 b 2 c 2 2bc cos A or cos A b2 c 2 a 2. etion 6. Lw of osines 59 etion 6. Lw of osines If is ny oblique tringle with sides, b, nd, the following equtions re vlid. () b b os or os b b (b) b os or os b () b b os or os b b You should be ble to

Διαβάστε περισσότερα

10/3/ revolution = 360 = 2 π radians = = x. 2π = x = 360 = : Measures of Angles and Rotations

10/3/ revolution = 360 = 2 π radians = = x. 2π = x = 360 = : Measures of Angles and Rotations //.: Measures of Angles and Rotations I. Vocabulary A A. Angle the union of two rays with a common endpoint B. BA and BC C. B is the vertex. B C D. You can think of BA as the rotation of (clockwise) with

Διαβάστε περισσότερα

is like multiplying by the conversion factor of. Dividing by 2π gives you the

is like multiplying by the conversion factor of. Dividing by 2π gives you the Chapter Graphs of Trigonometric Functions Answer Ke. Radian Measure Answers. π. π. π. π. 7π. π 7. 70 8. 9. 0 0. 0. 00. 80. Multipling b π π is like multipling b the conversion factor of. Dividing b 0 gives

Διαβάστε περισσότερα

Parametrized Surfaces

Parametrized Surfaces Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some

Διαβάστε περισσότερα

CRASH COURSE IN PRECALCULUS

CRASH COURSE IN PRECALCULUS CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter

Διαβάστε περισσότερα

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2 Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the

Διαβάστε περισσότερα

If we restrict the domain of y = sin x to [ π 2, π 2

If we restrict the domain of y = sin x to [ π 2, π 2 Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the

Διαβάστε περισσότερα

Quantitative Aptitude 1 Algebraic Identities Answers and Explanations

Quantitative Aptitude 1 Algebraic Identities Answers and Explanations Quntittive ptitude lgebric Identities nswers nd Eplntions P- (S) d 5 6 b 7 c 8 b 9 c 0 d d 5 d 6 d 7 b 8 9 c 0 c c b 5 6 7 8 c 9 d 0 b d b b 5 6 b 7 c 8 b 9 c 0 d c c b c 5 d 6 c 7 d 8 b 9 c 50 b. Q +

Διαβάστε περισσότερα

11.4 Graphing in Polar Coordinates Polar Symmetries

11.4 Graphing in Polar Coordinates Polar Symmetries .4 Graphing in Polar Coordinates Polar Symmetries x axis symmetry y axis symmetry origin symmetry r, θ = r, θ r, θ = r, θ r, θ = r, + θ .4 Graphing in Polar Coordinates Polar Symmetries x axis symmetry

Διαβάστε περισσότερα

y(t) S x(t) S dy dx E, E E T1 T2 T1 T2 1 T 1 T 2 2 T 2 1 T 2 2 3 T 3 1 T 3 2... V o R R R T V CC P F A P g h V ext V sin 2 S f S t V 1 V 2 V out sin 2 f S t x 1 F k q K x q K k F d F x d V

Διαβάστε περισσότερα

Differential equations

Differential equations Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential

Διαβάστε περισσότερα

( )( ) La Salle College Form Six Mock Examination 2013 Mathematics Compulsory Part Paper 2 Solution

( )( ) La Salle College Form Six Mock Examination 2013 Mathematics Compulsory Part Paper 2 Solution L Slle ollege Form Si Mock Emintion 0 Mthemtics ompulsor Prt Pper Solution 6 D 6 D 6 6 D D 7 D 7 7 7 8 8 8 8 D 9 9 D 9 D 9 D 5 0 5 0 5 0 5 0 D 5. = + + = + = = = + = =. D The selling price = $ ( 5 + 00)

Διαβάστε περισσότερα

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Review Test MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Find the exact value of the expression. 1) sin - 11π 1 1) + - + - - ) sin 11π 1 ) ( -

Διαβάστε περισσότερα

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint 1. a) 5 points) Find the unit tangent and unit normal vectors T and N to the curve at the point P, π, rt) cost, t, sint ). b) 5 points) Find curvature of the curve at the point P. Solution: a) r t) sint,,

Διαβάστε περισσότερα

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

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) = Mock Eam 7 Mock Eam 7 Section A. Reference: HKDSE Math M 0 Q (a) ( + k) n nn ( )( k) + nk ( ) + + nn ( ) k + nk + + + A nk... () nn ( ) k... () From (), k...() n Substituting () into (), nn ( ) n 76n 76n

Διαβάστε περισσότερα

THE UNIVERSITY OF MALTA DEPARTMENT OF MATHEMATICS MATHEMATICAL FORMULAE

THE UNIVERSITY OF MALTA DEPARTMENT OF MATHEMATICS MATHEMATICAL FORMULAE THE UNIVERSITY OF MALTA DEPARTMENT OF MATHEMATICS MATHEMATICAL FORMULAE UNIVERSITY PRESS, MSIDA, MALTA 208 THE UNIVERSITY OF MALTA DEPARTMENT OF MATHEMATICS MATHEMATICAL FORMULAE UNIVERSITY PRESS, MSIDA,

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is Pg. 9. The perimeter is P = The area of a triangle is A = bh where b is the base, h is the height 0 h= btan 60 = b = b In our case b =, then the area is A = = 0. By Pythagorean theorem a + a = d a a =

Διαβάστε περισσότερα

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

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds! MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.

Διαβάστε περισσότερα

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD CHAPTER FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD EXERCISE 36 Page 66. Determine the Fourier series for the periodic function: f(x), when x +, when x which is periodic outside this rge of period.

Διαβάστε περισσότερα

Vidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a

Vidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a Per -.(D).() Vdymndr lsses Solutons to evson est Seres - / EG / JEE - (Mthemtcs) Let nd re dmetrcl ends of crcle Let nd D re dmetrcl ends of crcle Hence mnmum dstnce s. y + 4 + 4 6 Let verte (h, k) then

Διαβάστε περισσότερα

Review Exercises for Chapter 7

Review Exercises for Chapter 7 8 Chapter 7 Integration Techniques, L Hôpital s Rule, and Improper Integrals 8. For n, I d b For n >, I n n u n, du n n d, dv (a) d b 6 b 6 (b) (c) n d 5 d b n n b n n n d, v d 6 5 5 6 d 5 5 b d 6. b 6

Διαβάστε περισσότερα

MATH 150 Pre-Calculus

MATH 150 Pre-Calculus MATH 150 Pre-Calculus Fall, 014, WEEK 11 JoungDong Kim Week 11: 8A, 8B, 8C, 8D Chapter 8. Trigonometry Chapter 8A. Angles and Circles The size of an angle may be measured in revolutions (rev), in degree

Διαβάστε περισσότερα

CHAPTER 12: PERIMETER, AREA, CIRCUMFERENCE, AND 12.1 INTRODUCTION TO GEOMETRIC 12.2 PERIMETER: SQUARES, RECTANGLES,

CHAPTER 12: PERIMETER, AREA, CIRCUMFERENCE, AND 12.1 INTRODUCTION TO GEOMETRIC 12.2 PERIMETER: SQUARES, RECTANGLES, CHAPTER : PERIMETER, AREA, CIRCUMFERENCE, AND SIGNED FRACTIONS. INTRODUCTION TO GEOMETRIC MEASUREMENTS p. -3. PERIMETER: SQUARES, RECTANGLES, TRIANGLES p. 4-5.3 AREA: SQUARES, RECTANGLES, TRIANGLES p.

Διαβάστε περισσότερα

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)

Διαβάστε περισσότερα

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

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β 3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle

Διαβάστε περισσότερα

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

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =? Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: linear functions Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U

Διαβάστε περισσότερα

Derivations of Useful Trigonometric Identities

Derivations of Useful Trigonometric Identities Derivations of Useful Trigonometric Identities Pythagorean Identity This is a basic and very useful relationship which comes directly from the definition of the trigonometric ratios of sine and cosine

Διαβάστε περισσότερα

Section 7.7 Product-to-Sum and Sum-to-Product Formulas

Section 7.7 Product-to-Sum and Sum-to-Product Formulas Section 7.7 Product-to-Sum and Sum-to-Product Fmulas Objective 1: Express Products as Sums To derive the Product-to-Sum Fmulas will begin by writing down the difference and sum fmulas of the cosine function:

Διαβάστε περισσότερα

d dx x 2 = 2x d dx x 3 = 3x 2 d dx x n = nx n 1

d dx x 2 = 2x d dx x 3 = 3x 2 d dx x n = nx n 1 d dx x 2 = 2x d dx x 3 = 3x 2 d dx x n = nx n1 x dx = 1 2 b2 1 2 a2 a b b x 2 dx = 1 a 3 b3 1 3 a3 b x n dx = 1 a n +1 bn +1 1 n +1 an +1 d dx d dx f (x) = 0 f (ax) = a f (ax) lim d dx f (ax) = lim 0 =

Διαβάστε περισσότερα

Solution to Review Problems for Midterm III

Solution to Review Problems for Midterm III Solution to Review Problems for Mierm III Mierm III: Friday, November 19 in class Topics:.8-.11, 4.1,4. 1. Find the derivative of the following functions and simplify your answers. (a) x(ln(4x)) +ln(5

Διαβάστε περισσότερα

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1 Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the

Διαβάστε περισσότερα

ECE 468: Digital Image Processing. Lecture 8

ECE 468: Digital Image Processing. Lecture 8 ECE 468: Digital Image Processing Lecture 8 Prof. Sinisa Todorovic sinisa@eecs.oregonstate.edu 1 Image Reconstruction from Projections X-ray computed tomography: X-raying an object from different directions

Διαβάστε περισσότερα

List MF20. List of Formulae and Statistical Tables. Cambridge Pre-U Mathematics (9794) and Further Mathematics (9795)

List MF20. List of Formulae and Statistical Tables. Cambridge Pre-U Mathematics (9794) and Further Mathematics (9795) List MF0 List of Formulae and Statistical Tables Cambridge Pre-U Mathematics (979) and Further Mathematics (979) For use from 07 in all aers for the above syllabuses. CST7 Mensuration Surface area of shere

Διαβάστε περισσότερα

Review of Essential Skills- Part 1. Practice 1.4, page 38. Practise, Apply, Solve 1.7, page 57. Practise, Apply, Solve 1.

Review of Essential Skills- Part 1. Practice 1.4, page 38. Practise, Apply, Solve 1.7, page 57. Practise, Apply, Solve 1. Review of Essential Skills- Part Operations with Rational Numbers, page. (e) 8 Exponent Laws, page 6. (a) 0 + 5 0, (d) (), (e) +, 8 + (h) 5, 9. (h) x 5. (d) v 5 Expanding, Simplifying, and Factoring Algebraic

Διαβάστε περισσότερα

Section 9.2 Polar Equations and Graphs

Section 9.2 Polar Equations and Graphs 180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify

Διαβάστε περισσότερα

Trigonometry (4A) Trigonometric Identities. Young Won Lim 1/2/15

Trigonometry (4A) Trigonometric Identities. Young Won Lim 1/2/15 Trigonometry (4 Trigonometric Identities 1//15 Copyright (c 011-014 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License,

Διαβάστε περισσότερα

Aquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET

Aquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET Aquinas College Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE in Mathematics and Further Mathematics Mathematical

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

Appendix A. Curvilinear coordinates. A.1 Lamé coefficients. Consider set of equations. ξ i = ξ i (x 1,x 2,x 3 ), i = 1,2,3

Appendix A. Curvilinear coordinates. A.1 Lamé coefficients. Consider set of equations. ξ i = ξ i (x 1,x 2,x 3 ), i = 1,2,3 Appendix A Curvilinear coordinates A. Lamé coefficients Consider set of equations ξ i = ξ i x,x 2,x 3, i =,2,3 where ξ,ξ 2,ξ 3 independent, single-valued and continuous x,x 2,x 3 : coordinates of point

Διαβάστε περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- ----------------- Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin

Διαβάστε περισσότερα

1. If log x 2 y 2 = a, then dy / dx = x 2 + y 2 1] xy 2] y / x. 3] x / y 4] none of these

1. If log x 2 y 2 = a, then dy / dx = x 2 + y 2 1] xy 2] y / x. 3] x / y 4] none of these 1. If log x 2 y 2 = a, then dy / dx = x 2 + y 2 1] xy 2] y / x 3] x / y 4] none of these 1. If log x 2 y 2 = a, then x 2 + y 2 Solution : Take y /x = k y = k x dy/dx = k dy/dx = y / x Answer : 2] y / x

Διαβάστε περισσότερα

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2 ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =

Διαβάστε περισσότερα

Section 8.2 Graphs of Polar Equations

Section 8.2 Graphs of Polar Equations Section 8. Graphs of Polar Equations Graphing Polar Equations The graph of a polar equation r = f(θ), or more generally F(r,θ) = 0, consists of all points P that have at least one polar representation

Διαβάστε περισσότερα

) = ( 2 ) = ( -2 ) = ( -3 ) = ( 0. Solutions Key Spatial Reasoning. 225 Holt McDougal Geometry ARE YOU READY? PAGE 651

) = ( 2 ) = ( -2 ) = ( -3 ) = ( 0. Solutions Key Spatial Reasoning. 225 Holt McDougal Geometry ARE YOU READY? PAGE 651 CHAPTER 10 Solutions Key Spatial Reasoning ARE YOU READY? PAGE 651 1. D. C. A 4. E 5. b = AB = 5-0 = 5; h = - (-1 = 4 bh = (5(4 = 10 units A = 6. b = LM = 6 - (- = 8, h = KL = 7 - = 4 A = bh = (8(4 = units

Διαβάστε περισσότερα

Spherical Coordinates

Spherical Coordinates Spherical Coordinates MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011 Spherical Coordinates Another means of locating points in three-dimensional space is known as the spherical

Διαβάστε περισσότερα

Geodesic Equations for the Wormhole Metric

Geodesic Equations for the Wormhole Metric Geodesic Equations for the Wormhole Metric Dr R Herman Physics & Physical Oceanography, UNCW February 14, 2018 The Wormhole Metric Morris and Thorne wormhole metric: [M S Morris, K S Thorne, Wormholes

Διαβάστε περισσότερα

Integrals in cylindrical, spherical coordinates (Sect. 15.7)

Integrals in cylindrical, spherical coordinates (Sect. 15.7) Integrals in clindrical, spherical coordinates (Sect. 5.7 Integration in spherical coordinates. Review: Clindrical coordinates. Spherical coordinates in space. Triple integral in spherical coordinates.

Διαβάστε περισσότερα

Lifting Entry (continued)

Lifting Entry (continued) ifting Entry (continued) Basic planar dynamics of motion, again Yet another equilibrium glide Hypersonic phugoid motion Planar state equations MARYAN 1 01 avid. Akin - All rights reserved http://spacecraft.ssl.umd.edu

Διαβάστε περισσότερα

26 28 Find an equation of the tangent line to the curve at the given point Discuss the curve under the guidelines of Section

26 28 Find an equation of the tangent line to the curve at the given point Discuss the curve under the guidelines of Section SECTION 5. THE NATURAL LOGARITHMIC FUNCTION 5. THE NATURAL LOGARITHMIC FUNCTION A Click here for answers. S Click here for solutions. 4 Use the Laws of Logarithms to epand the quantit.. ln ab. ln c. ln

Διαβάστε περισσότερα

Solutions to Exercise Sheet 5

Solutions to Exercise Sheet 5 Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X

Διαβάστε περισσότερα

Second Order Partial Differential Equations

Second Order Partial Differential Equations Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y

Διαβάστε περισσότερα

AREAS AND LENGTHS IN POLAR COORDINATES. 25. Find the area inside the larger loop and outside the smaller loop

AREAS AND LENGTHS IN POLAR COORDINATES. 25. Find the area inside the larger loop and outside the smaller loop SECTIN 9. AREAS AND LENGTHS IN PLAR CRDINATES 9. AREAS AND LENGTHS IN PLAR CRDINATES A Click here for answers. S Click here for solutions. 8 Find the area of the region that is bounded by the given curve

Διαβάστε περισσότερα

Trigonometry 1.TRIGONOMETRIC RATIOS

Trigonometry 1.TRIGONOMETRIC RATIOS Trigonometry.TRIGONOMETRIC RATIOS. If a ray OP makes an angle with the positive direction of X-axis then y x i) Sin ii) cos r r iii) tan x y (x 0) iv) cot y x (y 0) y P v) sec x r (x 0) vi) cosec y r (y

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

Navigation Mathematics: Kinematics (Coordinate Frame Transformation) EE 565: Position, Navigation and Timing

Navigation Mathematics: Kinematics (Coordinate Frame Transformation) EE 565: Position, Navigation and Timing Lecture Navigation Mathematics: Kinematics (Coordinate Frame Transformation) EE 565: Position, Navigation and Timing Lecture Notes Update on Feruary 20, 2018 Aly El-Osery and Kevin Wedeward, Electrical

Διαβάστε περισσότερα

Section 8.3 Trigonometric Equations

Section 8.3 Trigonometric Equations 99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.

Διαβάστε περισσότερα

d 2 y dt 2 xdy dt + d2 x

d 2 y dt 2 xdy dt + d2 x y t t ysin y d y + d y y t z + y ty yz yz t z y + t + y + y + t y + t + y + + 4 y 4 + t t + 5 t Ae cos + Be sin 5t + 7 5 y + t / m_nadjafikhah@iustacir http://webpagesiustacir/m_nadjafikhah/courses/ode/fa5pdf

Διαβάστε περισσότερα

Double Integrals, Iterated Integrals, Cross-sections

Double Integrals, Iterated Integrals, Cross-sections Chapter 14 Multiple Integrals 1 Double Integrals, Iterated Integrals, Cross-sections 2 Double Integrals over more general regions, Definition, Evaluation of Double Integrals, Properties of Double Integrals

Διαβάστε περισσότερα

Math221: HW# 1 solutions

Math221: HW# 1 solutions Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin

Διαβάστε περισσότερα

PARTIAL NOTES for 6.1 Trigonometric Identities

PARTIAL NOTES for 6.1 Trigonometric Identities PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot

Διαβάστε περισσότερα

2x 2 y x 4 +y 2 J (x, y) (0, 0) 0 J (x, y) = (0, 0) I ϕ(t) = (t, at), ψ(t) = (t, t 2 ), a ÑL<ÝÉ b, ½-? A? 2t 2 at t 4 +a 2 t 2 = lim

2x 2 y x 4 +y 2 J (x, y) (0, 0) 0 J (x, y) = (0, 0) I ϕ(t) = (t, at), ψ(t) = (t, t 2 ), a ÑL<ÝÉ b, ½-? A? 2t 2 at t 4 +a 2 t 2 = lim 9çB$ø`çü5 (-ç ) Ch.Ch4 b. è. [a] #8ƒb f(x, y) = { x y x 4 +y J (x, y) (, ) J (x, y) = (, ) I ϕ(t) = (t, at), ψ(t) = (t, t ), a ÑL

Διαβάστε περισσότερα

SOLUTIONS & ANSWERS FOR KERALA ENGINEERING ENTRANCE EXAMINATION-2018 PAPER II VERSION B1

SOLUTIONS & ANSWERS FOR KERALA ENGINEERING ENTRANCE EXAMINATION-2018 PAPER II VERSION B1 SOLUTIONS & ANSWERS FOR KERALA ENGINEERING ENTRANCE EXAMINATION-8 PAPER II VERSION B [MATHEMATICS]. Ans: ( i) It is (cs5 isin5 ) ( i). Ans: i z. Ans: i i i The epressin ( i) ( ). Ans: cs i sin cs i sin

Διαβάστε περισσότερα

Answer sheet: Third Midterm for Math 2339

Answer sheet: Third Midterm for Math 2339 Answer sheet: Third Midterm for Math 339 November 3, Problem. Calculate the iterated integrals (Simplify as much as possible) (a) e sin(x) dydx y e sin(x) dydx y sin(x) ln y ( cos(x)) ye y dx sin(x)(lne

Διαβάστε περισσότερα

Problem 3.1 Vector A starts at point (1, 1, 3) and ends at point (2, 1,0). Find a unit vector in the direction of A. Solution: A = 1+9 = 3.

Problem 3.1 Vector A starts at point (1, 1, 3) and ends at point (2, 1,0). Find a unit vector in the direction of A. Solution: A = 1+9 = 3. Problem 3.1 Vector A starts at point (1, 1, 3) and ends at point (, 1,0). Find a unit vector in the direction of A. Solution: A = ˆx( 1)+ŷ( 1 ( 1))+ẑ(0 ( 3)) = ˆx+ẑ3, A = 1+9 = 3.16, â = A A = ˆx+ẑ3 3.16

Διαβάστε περισσότερα

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

Approximation of distance between locations on earth given by latitude and longitude Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth

Διαβάστε περισσότερα

Problem 3.16 Given B = ˆx(z 3y) +ŷ(2x 3z) ẑ(x+y), find a unit vector parallel. Solution: At P = (1,0, 1), ˆb = B

Problem 3.16 Given B = ˆx(z 3y) +ŷ(2x 3z) ẑ(x+y), find a unit vector parallel. Solution: At P = (1,0, 1), ˆb = B Problem 3.6 Given B = ˆxz 3y) +ŷx 3z) ẑx+y), find a unit vector parallel to B at point P =,0, ). Solution: At P =,0, ), B = ˆx )+ŷ+3) ẑ) = ˆx+ŷ5 ẑ, ˆb = B B = ˆx+ŷ5 ẑ = ˆx+ŷ5 ẑ. +5+ 7 Problem 3.4 Convert

Διαβάστε περισσότερα

Notations. Primary definition. Specific values. General characteristics. Series representations. Traditional name. Traditional notation

Notations. Primary definition. Specific values. General characteristics. Series representations. Traditional name. Traditional notation Pi Notations Traditional name Π Traditional notation Π Mathematica StandardForm notation Pi Primary definition.3... Π Specific values.3.3.. Π 3.5965358979338663383795889769399375589795937866868998683853

Διαβάστε περισσότερα

Electromagnetic Waves I

Electromagnetic Waves I Electromgnetic Wves I Jnury, 03. Derivtion of wve eqution of string. Derivtion of EM wve Eqution in time domin 3. Derivtion of the EM wve Eqution in phsor domin 4. The complex propgtion constnt 5. The

Διαβάστε περισσότερα

Quadratic Expressions

Quadratic Expressions Quadratic Expressions. The standard form of a quadratic equation is ax + bx + c = 0 where a, b, c R and a 0. The roots of ax + bx + c = 0 are b ± b a 4ac. 3. For the equation ax +bx+c = 0, sum of the roots

Διαβάστε περισσότερα

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =

Διαβάστε περισσότερα

Lifting Entry 2. Basic planar dynamics of motion, again Yet another equilibrium glide Hypersonic phugoid motion MARYLAND U N I V E R S I T Y O F

Lifting Entry 2. Basic planar dynamics of motion, again Yet another equilibrium glide Hypersonic phugoid motion MARYLAND U N I V E R S I T Y O F ifting Entry Basic planar dynamics of motion, again Yet another equilibrium glide Hypersonic phugoid motion MARYAN 1 010 avid. Akin - All rights reserved http://spacecraft.ssl.umd.edu ifting Atmospheric

Διαβάστε περισσότερα

Solutions 3. February 2, Apply composite Simpson s rule with m = 1, 2, 4 panels to approximate the integrals:

Solutions 3. February 2, Apply composite Simpson s rule with m = 1, 2, 4 panels to approximate the integrals: s Februry 2, 216 1 Exercise 5.2. Apply composite Simpson s rule with m = 1, 2, 4 pnels to pproximte the integrls: () x 2 dx = 1 π/2, (b) cos(x) dx = 1, (c) e x dx = e 1, nd report the errors. () f(x) =

Διαβάστε περισσότερα

1 Adda247 No. 1 APP for Banking & SSC Preparation Website:store.adda247.com

1 Adda247 No. 1 APP for Banking & SSC Preparation Website:store.adda247.com Adda47 No. APP for Banking & SSC Preparation Website:store.adda47.com Email:ebooks@adda47.com S. Ans.(d) Given, x + x = 5 3x x + 5x = 3x x [(x + x ) 5] 3 (x + ) 5 = 3 0 5 = 3 5 x S. Ans.(c) (a + a ) =

Διαβάστε περισσότερα

F19MC2 Solutions 9 Complex Analysis

F19MC2 Solutions 9 Complex Analysis F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at

Διαβάστε περισσότερα

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C By Tom Irvine Email: tomirvine@aol.com August 6, 8 Introduction The obective is to derive a Miles equation which gives the overall response

Διαβάστε περισσότερα

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits. EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.

Διαβάστε περισσότερα

Probability and Random Processes (Part II)

Probability and Random Processes (Part II) Probability and Random Processes (Part II) 1. If the variance σ x of d(n) = x(n) x(n 1) is one-tenth the variance σ x of a stationary zero-mean discrete-time signal x(n), then the normalized autocorrelation

Διαβάστε περισσότερα

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ. Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +

Διαβάστε περισσότερα

MATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81

MATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 We know that KA = A If A is n th Order 3AB =3 3 A. B = 27 1 3 = 81 3 2. If A= 2 1 0 0 2 1 then

Διαβάστε περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.S. 430 Assignment 6, Sample Solutions C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order

Διαβάστε περισσότερα

Math 6 SL Probability Distributions Practice Test Mark Scheme

Math 6 SL Probability Distributions Practice Test Mark Scheme Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry

Διαβάστε περισσότερα

Trigonometry Functions (5B) Young Won Lim 7/24/14

Trigonometry Functions (5B) Young Won Lim 7/24/14 Trigonometry Functions (5B 7/4/14 Copyright (c 011-014 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version

Διαβάστε περισσότερα

SPECIAL FUNCTIONS and POLYNOMIALS

SPECIAL FUNCTIONS and POLYNOMIALS SPECIAL FUNCTIONS and POLYNOMIALS Gerard t Hooft Stefan Nobbenhuis Institute for Theoretical Physics Utrecht University, Leuvenlaan 4 3584 CC Utrecht, the Netherlands and Spinoza Institute Postbox 8.195

Διαβάστε περισσότερα

16. 17. r t te 2t i t 1. 18 19 Find the derivative of the vector function. 19. r t e t cos t i e t sin t j ln t k. 31 33 Evaluate the integral.

16. 17. r t te 2t i t 1. 18 19 Find the derivative of the vector function. 19. r t e t cos t i e t sin t j ln t k. 31 33 Evaluate the integral. SECTION.7 VECTOR FUNCTIONS AND SPACE CURVES.7 VECTOR FUNCTIONS AND SPACE CURVES A Click here for answers. S Click here for soluions. Copyrigh Cengage Learning. All righs reserved.. Find he domain of he

Διαβάστε περισσότερα

ECE 308 SIGNALS AND SYSTEMS FALL 2017 Answers to selected problems on prior years examinations

ECE 308 SIGNALS AND SYSTEMS FALL 2017 Answers to selected problems on prior years examinations ECE 308 SIGNALS AND SYSTEMS FALL 07 Answers to selected problems on prior years examinations Answers to problems on Midterm Examination #, Spring 009. x(t) = r(t + ) r(t ) u(t ) r(t ) + r(t 3) + u(t +

Διαβάστε περισσότερα

Κλασσική Θεωρία Ελέγχου

Κλασσική Θεωρία Ελέγχου ΑΡΙΣΤΟΤΕΛΕΙΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΘΕΣΣΑΛΟΝΙΚΗΣ ΑΝΟΙΧΤΑ ΑΚΑΔΗΜΑΙΚΑ ΜΑΘΗΜΑΤΑ Ενότητα 5: Ο μετασχηματισμός Laplace Νίκος Καραμπετάκης Άδειες Χρήσης Το παρόν εκπαιδευτικό υλικό υπόκειται σε άδειες χρήσης Creative

Διαβάστε περισσότερα

ΚΕΦΑΛΑΙΟ 2. Περιγραφή της Κίνησης. 2.1 Κίνηση στο Επίπεδο

ΚΕΦΑΛΑΙΟ 2. Περιγραφή της Κίνησης. 2.1 Κίνηση στο Επίπεδο ΚΕΦΑΛΑΙΟ 2 Περιγραφή της Κίνησης Στο κεφάλαιο αυτό θα δείξουμε πώς να προγραμματίσουμε απλές εξισώσεις τροχιάς ενός σωματιδίου και πώς να κάνουμε βασική ανάλυση των αριθμητικών αποτελεσμάτων. Χρησιμοποιούμε

Διαβάστε περισσότερα

Lecture 26: Circular domains

Lecture 26: Circular domains Introductory lecture notes on Partial Differential Equations - c Anthony Peirce. Not to be copied, used, or revised without eplicit written permission from the copyright owner. 1 Lecture 6: Circular domains

Διαβάστε περισσότερα