GAYAZA HIGH SCHOOL MATHS SEMINAR- APPLIED MATHS SOLUTIONS
|
|
- Ευτροπια Δασκαλοπούλου
- 5 χρόνια πριν
- Προβολές:
Transcript
1 PROBABILITY AND STATISTICS. (a) Let X be a r.v number of games won. X~B(6, ) (i) Expectation, E(X) = np 6x = 4 (ii) P(X ) = P(X < ) = (P(X = ) + P(= 0)) = C x x C0x x (b) Let X be a r.v number outside the tolerance limit. Since n >00, then X~N(np, npq) μ = np = 00x0.5 = 0 and σ = npq = 00x0.5x0.85 =.5 (i) P(X > ) = P(X.5) = P (Z >.5 0 ) = P(Z >.79) = (.79).5 = = (ii) P(0 X 0) = P(9.5 < X < 0.5) = P ( = P(.4 < Z < 0.05) = (0.05) + (.4) = = < Z < ) Marks Frequency Mid fx Cumulative fx (f) point(x) frequency(c.f) 5-< < < < < < < < < f=5 fx=59 fx =006 COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
2 (a) (i) Var ( x) Mode 40 x0 4 (ii) (b) (i) From the graph below, 68 th percentile= x5 th 85 value = 5.5 th value (ii) Number of students who scored above 47% = (5-65) =60 students COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
3 GAYAZA HIGH SCHOOL MATHS SEMINAR- APPLIED MATHS SOLUTIONS COMPILED BY: THEODE NIYIRINDA. TEL: / Page
4 . (a) (i) P(AuB) = P(A) + P(B) P(AnB); but P(AnB)= P(A)xP(A/B) = x (0.) 0.6 = x y - (0.)x x y 6 8x 0y 4x 5y...() (ii) P(BuC) = P(B) + P(C) 0.9 y ( x y) 0.9 y x 9 0y 0x...( ) Solving equation () and () simultaneously gives; x 0.5, y 0. For independent events P(AnB) = P(A) x P(B) P(AnB) = 0.5x0. = 0. and P(A)xP(B) = 0.5x0. = 0.. Hence A and B are independent events. (b) (i) P(AuB) = P(A) + P(B) P(AnB) P( B). P( B) P( B) 6 P( AnB) P( A) xp( B) P A P( B) B P( A) P( A) (ii) P B P ( B na) P( B ) (iii) A P( A) P ( B) 4 x x d 4. (i) f ( x) dx allx ax ( d x) dx a d a a( 4d )...( i) E ( X ) x. f ( x) dx 0.6 x. ax ( d x) dx allx x x 0.6 a d 0.6 a d 4 5 a(5d 4)...( ii) Divide equation (ii) by equation (i) a(5d 4) 5d 4 4d d From equation (i) a a(4d ) (b) P(0.9 x ) 0.9 x 4 x x ( x) dx COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 4
5 5. (a) (i) P(X = x) X P(X = x) = k X X 4 P(x=x) k k k k But k + K + K + K = k 44 k = (ii) Var(x) = Var(X) = [E(X ) (E(X) )] But E(X) = ( k) + ( k ) + 4 ( k) + (4 k ) = 5k = 60 and k k k E( x ) k 4 4k Hence Var (x) 94x b) P(X = x) = all x K + k+ k+..+nk = K(+++ +n) = K( n (n+)) = K = n(n+).(i) Also E ( x) x. P( X x) allx K + (K) + (K) +...+n(nk) = 5 K( n ) = 5 K( n(n+)(n+) ) = 5 6 Substituting K from equation (i) n(n+) x(n(n+)(n+) 6 ) = 5 4n + = 0, 4n = 8, n = 7 Hence k =, k = 7(8) 8 COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 5
6 ii) Var( x ) Var( x) 4E ( x ) E( x) x P(X=x) x X.P(X=x) X. P( X x) 8 Hence Var ( x) (a) -<x<0; f(-) = k(-+)=k, f(0) = k(0+) = k 0 <x<; f(0)=f() = k (5 ) (5 ) <x<; f ( ) k k ; f ( ) k k f(x) f(x)=k(x+) k f(x)= k f(x)=k (5- x) k - 0 x Area under the graph = ( kx 4) k(4 ) (b) t F ( x) f ( x) dx k COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 6
7 F( t) x 0; t F ( x) 0 x ; ( x ) dx x 4x 4 F t) F(0) dx 0 t x x t F( 0) t t 4x ( F( t) 4t F ( x) 4x F( ) 7 t 0 4t t 4t x ; x F t F 5 ( ) () dx F( t) 7 t x 5x t 7 F ( x) 0x x 5 F() 6 Hence t 5t 5 6 0t t 5 F(x) = x 0 4x 0x x 5 6 { 4x (c) P0.5 x P(0.5 X nx x X = 6 X<- -<X<0 <X< X> 0<X< ) P( x ) F() F() P( x ) F() 0x 5 4x 4x COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 7
8 7. Let X be a r.v weight of the cabbage X~N(50, 6 ) (a) (i) P( 48 X 57.4) P Z P 0. Z. 6 6 (b) P(48 <X <57.4) = (.) + (0.) = = (ii) P ( X 46.) P Z P( Z 0.65) 6 Hence P ( X 46.) 0.5 (0.65) y 50 P P ( Z Z) 0. where Z y 50 6Z 6 (c) X y 0. COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 8
9 From critical table, Z =.8 Hence y = 50 +6(.8) = g 8. (a) Let X be a r.v number of students with blue eyes. X~B (n, 5 ) P ( X 0) n 0 n 0 C x n 4 x log 5 n log(0.00) n Hence the least value is 0 log(0.00) n 4 log 5 (b) Let events A and B be John wins the first and second game respectively. P ( A) 0., P ( A ) 0. 7, P B 0. 6, A P B 0. 5 A A P( AnB) B P( B) P( AnB) P( A nb) P( A) xp B P( A ) xp B P( B) A A P but = 0.x x0.5 = x0.6 Hence P A B 0.85 (d) Let R and A be events Robot and aeroplane respectively; Dan 0 5 P ( RD ), P( AD ) 5 5 Emma 7 7 x P( RE ), P( AE ) x 7 x 4 x 4 7 P( RD xre ) 8 Hence 7 7 x ( x 4) x 8 x 4 8 COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 9
10 9. MECHANICS Weight α Area W=gA, where g is a constant Portion Area Weight Position of c.o.g from OA and OE Rectangle, OABE (4x6) =4cm 4g ( 7, 8) Triangle, CBD x x9 = 49.5cm 49.5g 0, Remainder (4 49.5) = 74.5g ( x, y ) 74.5cm Taking moments about O, x 7 x g 4g 49.5g y 8 y x y 8.78 Position of c.o.g is (5.980, 8.78) (b) COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 0
11 8.78 Tanθ= Θ= Tanα= 4 =48.8 Hence OB makes an angle of ( ) = 8.9 with the vertical 0. (a) Impulse = Change in momentum 6 4 F.t = m(v-u) x.5 v 9 8 v v Hence final velocity, v 0.5i 4.5 j. 5k (b) Let the body have mass, mkg, natural length, l and displaced by x equilibrium T l 0.5m x In equilibrium; e T = mg, but T l (0.5) mg... ( i) l mg COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
12 (0.5 When displaced by x; restoring force is; mg T ma where T l ( 0.5) (0.5 x) x ma ma a x..(ii) l l l ml Compare eqn(ii) by a x mgl From equation (i) 0.5 g=0ms - Hence T 5 seconds 5. (a) Let the acceleration of the car be a ms - But T ml ml x) ml(0.5) T ; mgl Sinα= 0 Along the plane; 900 (400000g sin) 000a x0x a 0.5ms 0 000a 08x000 U 0ms V = 0 ms - 60x60 Using V = U +as 0 = 0 +(-0.5)S Hence distance travelled is S = 900m COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
13 (b) Work done= F. AB but F = ( 5 4 ) + ( 0 7 ) + ( 0 ) = ( 4 5 ) N Distance, AB = ( 4) ( ) = ( 6) m Hence Work done =( ). ( 6) = (4x4 + x6 + 5x) = 8 Joules 5. Let the body make an angle, θ Distance = xr 60 (r ) xr Using V U as r V rg ( g)( h) But h r( cos60) r V rg ( g)( ) rg Hence V rgms (0.) rg Resolving along the radius, R 0x9.8( cos60) 49N R 0.gCos60 r COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
14 . (a) Resolving along the plane; FCos 0 gsin FCos 0.5R 0 but R FSin0 gcos0 FSin0 gcos gsin x9.8(0.5cos0 Sin0) F N Cos0 0.5Sin0 0 5 Cos (b) (i) Resultant force, F Sin Taking moment about point O, G = 8x 4x = 8Nm Let the line of action of the resultant force act at a point (x, y) x y Momemnt of the resultant is G 8x 7 y 7 8 But G = G ; Hence 8x 7y = 8 (ii) The line crosses C at a point when x = 0. -7y = 8 8 y Hence it crosses at a 7 point 8 cm below point C 7 COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 4
15 4. Whole system Resolving vertically in equilibrium, R R W 5W 6W...( i) A C Taking moments about point A R C 4R R x4bcos45 C W 5W 6W C 4W WxbCos45 From equation (i) R A 6W 4W W Splitting the joint at B 5WxbCos45 COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 5
16 Considering rod BC; Taking moments at the hinge B; 4wxbCos45 8W T tan 45 TxbSin45 5W W T Resolving on rod BC; 5WxbCos 45 Vertically; Y+4W = 5W Y W Horizontally: X T W W W W Hence reaction is R X Y W 4 Let the direction of the reaction act at θ to the horizontal, 5. Y W Tan. 7 X W a m/s - T T T am/s - g 5g (i) Using F = ma For 5Kg mass; 5g-T=5a () For kg mass; T-g=a T g = a...() COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 6
17 Adding () and () 4g = 6a a g x ms (ii) From equation () T = 5x9.8 5x6.5 = 6.5N s ut at s 0 x.5 x6.5x(.5) 7. 50N (iii) 6. Usinθ U y θ z X Horizontal displacement; X = (Ucosθ)t Ucosθ t x U cos..() Vertical displacement; y U sin. t gt () Put t from. () in () x x y U sin. g U cos U cos Hence y = xtanθ gx u ( + tan θ) gx gx Sec y x tan y x tan U Cos U COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 7
18 (b) U = 0 g y 40m Ɵ 40m x For the particle to clear the tower; y x40 ( tan 40tan x tan 8( tan ) 40 40tan 8tan 48 0 tan 5tan 6 0 tan tan 0 ) 40 tan 0 or tan 0 tan 0r tan Hence tan NUMERICAL ANALYSIS 7. (a) x Sinx ln x From graph x. 5 root COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 8
19 COMPILED BY: THEODE NIYIRINDA. TEL: / Page 9
20 (b) let f ( x) Sinx ln x x ( n) x n f ( Sinxn ln x Cosxn xn x) Cosx x n Using x. 5 x x o Sin(.5) ln(.5).5.94 Cos(.5).5 Sin(.94) ln(.94).94.9 Cos(.94).94 x x Hence x. 9 root 8. (a) From the graph on the next page, there is a positive relationship between mock and final mark (b) Mock Final R m R F d d = 9.5 Spearman s Correlation coefficient, ρ = 6x9.5 7(7 ) = Comment: There is a high positive correlation between the Mock and Final mark COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 0
21 GAYAZA HIGH SCHOOL MATHS SEMINAR- APPLIED MATHS SOLUTIONS COMPILED BY: THEODE NIYIRINDA. TEL: / Page
22 9. True value= X Y; X=x± x and Y=y± y (X Y) max =X maxy max =(x+ x) (y+ y) =(x +x x+ x )(y+ y) = (x y+ xxy+ x y+ yx + x yx + x y) (X Y) min = X miny min = (x x) (y y) = (x x x + x )(y y) Error= = (x y xxy + x y yx + x yx x y) (Max limit min limit) = x y+ xxy+ x y+ yx + x yx+ x y x y+ xxy x y+ yx x yx+ x y = 4 xxy + yx + x y Error = xy x + x y + x y For maximum error; if x and y are very small then, x y 0 Error= xy x + x y Error = xy x + x y xy x + x y Hence Max error = xy x + x y Max limit= x max y max = ( ) ( ) =.484 Min limit=x min y min = ( ) ( ) =.0989 Limits are [.0989,.484] or (.0989 x y.484) 0. (a) COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
23 A = pqsinα da dq = dp dα (psinα + q sin α + pqcosα ) dq dq Multiplying through by dq da = (p sin α dq + q sinα dp + pqcosα dα) da = (psinα dq + qsinα dp + pq cosα dα) da { psinα dq + qsinα dp + pqcosαdα } Maximum possible error = { psinα dq + qsinα dp + pqcosα dα } (ii) dp = 0.05 dq = 0.05 dα = 0.5 Error = π {4.5x sin 0x x sin 0x x8.4 cos 0x0.5x } 80 = Exact Area = sin 0 = 9.45 sq units %age error = = 6.4 (b) e (.679) = e (7.0) = 0.05 e () = 0.5 e (5.48) = Let.679 P P max = =.859 P min = 7.05 = The range is from 0.87 P.859 or 0.87,.859 COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page
24 . (a) h 0. 4 Let y x ln x 6 x, y5 y,..., y Sum y o 4 x ln xdx x x (b) Exact value; x x ln xdx ln x x. dx x x x x ln xdx ln x 9 x ln x x () ln () ln Hence x ln xdx Error = Therefore; % error = 0.05 x00 = Error can be reduced by increasing the number of sub-intervals or number of ordinates COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 4
25 . (i) START Read: a, b, c d = b 4ac Is d o? X = X = b i d a b i d a X = b d a X = b+ d a Print :X, X STOP (ii) d x x -6 i i For any inquiries feel free to drop me a line on contacts below COMPILED BY: THEODE NIYIRINDA. TEL: / niyirinda0@yahoo.com Page 5
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 περισσότεραHomework 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 περισσότεραMock 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 περισσότεραSolution 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 περισσότεραCHAPTER 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 περισσότεραSecond 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 περισσότεραAnswers - Worksheet A ALGEBRA PMT. 1 a = 7 b = 11 c = 1 3. e = 0.1 f = 0.3 g = 2 h = 10 i = 3 j = d = k = 3 1. = 1 or 0.5 l =
C ALGEBRA Answers - Worksheet A a 7 b c d e 0. f 0. g h 0 i j k 6 8 or 0. l or 8 a 7 b 0 c 7 d 6 e f g 6 h 8 8 i 6 j k 6 l a 9 b c d 9 7 e 00 0 f 8 9 a b 7 7 c 6 d 9 e 6 6 f 6 8 g 9 h 0 0 i j 6 7 7 k 9
Διαβάστε περισσότεραANSWERSHEET (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 περισσότεραCHAPTER 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 περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραMatrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Διαβάστε περισσότεραReview 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 περισσότεραInverse 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 περισσότεραSection 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 περισσότεραTrigonometric 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 περισσότερα2. 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 περισσότεραMath 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 περισσότεραPg 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 περισσότερα9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr
9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values
Διαβάστε περισσότερα1. 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 περισσότεραAreas 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 περισσότεραSCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Διαβάστε περισσότεραSOLUTIONS & 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 περισσότεραLifting 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 περισσότεραAreas 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 περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
Διαβάστε περισσότεραDifferentiation exercise show differential equation
Differentiation exercise show differential equation 1. If y x sin 2x, prove that x d2 y 2 2 + 2y x + 4xy 0 y x sin 2x sin 2x + 2x cos 2x 2 2cos 2x + (2 cos 2x 4x sin 2x) x d2 y 2 2 + 2y x + 4xy (2x cos
Διαβάστε περισσότερα3.4 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 περισσότερα1 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 περισσότεραis 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 περισσότεραSolutions 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 περισσότεραCRASH 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 περισσότεραCHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Διαβάστε περισσότεραStatistics 104: Quantitative Methods for Economics Formula and Theorem Review
Harvard College Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Tommy MacWilliam, 13 tmacwilliam@college.harvard.edu March 10, 2011 Contents 1 Introduction to Data 5 1.1 Sample
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότεραk A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
Διαβάστε περισσότερα1 String with massive end-points
1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε
Διαβάστε περισσότεραRectangular 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 περισσότεραSection 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 περισσότεραReview 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 περισσότεραPhysicsAndMathsTutor.com
PhysicsAndMathsTutor.com June 2005 1. A car of mass 1200 kg moves along a straight horizontal road. The resistance to motion of the car from non-gravitational forces is of constant magnitude 600 N. The
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Διαβάστε περισσότεραb. 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 περισσότεραEE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
Διαβάστε περισσότεραReminders: 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 περισσότεραExercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
Διαβάστε περισσότεραDERIVATION 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 περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr (T t N n) Pr (max (X 1,..., X N ) t N n) Pr (max
Διαβάστε περισσότεραProbability 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 περισσότεραD Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Διαβάστε περισσότεραthe total number of electrons passing through the lamp.
1. A 12 V 36 W lamp is lit to normal brightness using a 12 V car battery of negligible internal resistance. The lamp is switched on for one hour (3600 s). For the time of 1 hour, calculate (i) the energy
Διαβάστε περισσότεραCHAPTER 70 DOUBLE AND TRIPLE INTEGRALS. 2 is integrated with respect to x between x = 2 and x = 4, with y regarded as a constant
CHAPTER 7 DOUBLE AND TRIPLE INTEGRALS EXERCISE 78 Page 755. Evaluate: dxd y. is integrated with respect to x between x = and x =, with y regarded as a constant dx= [ x] = [ 8 ] = [ ] ( ) ( ) d x d y =
Διαβάστε περισσότεραMathCity.org Merging man and maths
MathCity.org Merging man and maths Exercise 10. (s) Page Textbook of Algebra and Trigonometry for Class XI Available online @, Version:.0 Question # 1 Find the values of sin, and tan when: 1 π (i) (ii)
Διαβάστε περισσότεραQuadratic 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 περισσότερα6.4 Superposition of Linear Plane Progressive Waves
.0 - Marine Hydrodynamics, Spring 005 Lecture.0 - Marine Hydrodynamics Lecture 6.4 Superposition of Linear Plane Progressive Waves. Oblique Plane Waves z v k k k z v k = ( k, k z ) θ (Looking up the y-ais
Διαβάστε περισσότερα( ) 2 and compare to M.
Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8
Διαβάστε περισσότεραFourier Analysis of Waves
Exercises for the Feynman Lectures on Physics by Richard Feynman, Et Al. Chapter 36 Fourier Analysis of Waves Detailed Work by James Pate Williams, Jr. BA, BS, MSwE, PhD From Exercises for the Feynman
Διαβάστε περισσότεραPARTIAL 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 περισσότεραEE1. Solutions of Problems 4. : a) f(x) = x 2 +x. = (x+ǫ)2 +(x+ǫ) (x 2 +x) ǫ
EE Solutions of Problems 4 ) Differentiation from first principles: f (x) = lim f(x+) f(x) : a) f(x) = x +x f(x+) f(x) = (x+) +(x+) (x +x) = x+ + = x++ f(x+) f(x) Thus lim = lim x++ = x+. b) f(x) = cos(ax),
Διαβάστε περισσότεραAnswers to practice exercises
Answers to practice exercises Chapter Exercise (Page 5). 9 kg 2. 479 mm. 66 4. 565 5. 225 6. 26 7. 07,70 8. 4 9. 487 0. 70872. $5, Exercise 2 (Page 6). (a) 468 (b) 868 2. (a) 827 (b) 458. (a) 86 kg (b)
Διαβάστε περισσότεραPractice 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*H31123A0228* 1. (a) Find the value of at the point where x = 2 on the curve with equation. y = x 2 (5x 1). (6)
C3 past papers 009 to 01 physicsandmathstutor.comthis paper: January 009 If you don't find enough space in this booklet for your working for a question, then pleasecuse some loose-leaf paper and glue it
Διαβάστε περισσότεραSpherical 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 περισσότερα1. (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 περισσότερα1. Ηλεκτρικό μαύρο κουτί: Αισθητήρας μετατόπισης με βάση τη χωρητικότητα
IPHO_42_2011_EXP1.DO Experimental ompetition: 14 July 2011 Problem 1 Page 1 of 5 1. Ηλεκτρικό μαύρο κουτί: Αισθητήρας μετατόπισης με βάση τη χωρητικότητα Για ένα πυκνωτή χωρητικότητας ο οποίος είναι μέρος
Διαβάστε περισσότεραd 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 περισσότεραAnswer 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 περισσότεραST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Διαβάστε περισσότεραUDZ Swirl diffuser. Product facts. Quick-selection. Swirl diffuser UDZ. Product code example:
UDZ Swirl diffuser Swirl diffuser UDZ, which is intended for installation in a ventilation duct, can be used in premises with a large volume, for example factory premises, storage areas, superstores, halls,
Διαβάστε περισσότεραDESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Διαβάστε περισσότεραwave energy Superposition of linear plane progressive waves Marine Hydrodynamics Lecture Oblique Plane Waves:
3.0 Marine Hydrodynamics, Fall 004 Lecture 0 Copyriht c 004 MIT - Department of Ocean Enineerin, All rihts reserved. 3.0 - Marine Hydrodynamics Lecture 0 Free-surface waves: wave enery linear superposition,
Διαβάστε περισσότεραDETERMINATION OF DYNAMIC CHARACTERISTICS OF A 2DOF SYSTEM. by Zoran VARGA, Ms.C.E.
DETERMINATION OF DYNAMIC CHARACTERISTICS OF A 2DOF SYSTEM by Zoran VARGA, Ms.C.E. Euro-Apex B.V. 1990-2012 All Rights Reserved. The 2 DOF System Symbols m 1 =3m [kg] m 2 =8m m=10 [kg] l=2 [m] E=210000
Διαβάστε περισσότεραExample Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Διαβάστε περισσότεραSection 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 περισσότεραTrigonometry 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 περισσότεραFORMULAS FOR STATISTICS 1
FORMULAS FOR STATISTICS 1 X = 1 n Sample statistics X i or x = 1 n x i (sample mean) S 2 = 1 n 1 s 2 = 1 n 1 (X i X) 2 = 1 n 1 (x i x) 2 = 1 n 1 Xi 2 n n 1 X 2 x 2 i n n 1 x 2 or (sample variance) E(X)
Διαβάστε περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραEquations. 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 περισσότεραECE 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 περισσότεραMATHEMATICS. 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 περισσότεραProblem 1.1 For y = a + bx, y = 4 when x = 0, hence a = 4. When x increases by 4, y increases by 4b, hence b = 5 and y = 4 + 5x.
Appendix B: Solutions to Problems Problem 1.1 For y a + bx, y 4 when x, hence a 4. When x increases by 4, y increases by 4b, hence b 5 and y 4 + 5x. Problem 1. The plus sign indicates that y increases
Διαβάστε περισσότεραFinite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
Διαβάστε περισσότεραF19MC2 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 περισσότεραStrain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
Διαβάστε περισσότεραApproximation 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 περισσότεραProblem 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 περισσότεραBiostatistics for Health Sciences Review Sheet
Biostatistics for Health Sciences Review Sheet http://mathvault.ca June 1, 2017 Contents 1 Descriptive Statistics 2 1.1 Variables.............................................. 2 1.1.1 Qualitative........................................
Διαβάστε περισσότεραGraded Refractive-Index
Graded Refractive-Index Common Devices Methodologies for Graded Refractive Index Methodologies: Ray Optics WKB Multilayer Modelling Solution requires: some knowledge of index profile n 2 x Ray Optics for
Διαβάστε περισσότεραIf 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 περισσότεραParametrized 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 περισσότεραAREAS 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 περισσότεραDifferential 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 περισσότεραSolution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
Διαβάστε περισσότεραIf 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 περισσότεραMath221: 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 περισσότεραList 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 περισσότερα10/3/ 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 περισσότεραIntegrals 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 περισσότεραLifting 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 περισσότεραΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή
Διαβάστε περισσότερα