Inverse trigonometric functions & General Solution of Trigonometric Equations

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

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

Transcript

1 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 θ = 8/17 then cos θ = 15/17 GE 15/17. c is rejected. b is the answer. OR Let sin = θ then sin θ = Cos θ = 1 sin θ = 1 = = 17 then G E =sin = = = = = 2. The value of Tan ( - ) = a) b) c) d) Ans: b. Solution: Let tan = θ then tan θ = Tan ( - tan ) = Tan ( - θ) = = =. 3. The domain of the function f(x) = is a) 1 x 2 b) -1 x 2 c) 2 x 4 d) 1 x 5 Ans: a. Solution : we know that sin is defined when - 1 x x 4 1 x

2 4. If cos ( 3 ) = tan ( ) then x = a) 0 b) 1 c) -1 d) 0,1, -1 Ans: d. Solution : 1) inspection method GE is satisfied by all values. Hence ans is d. or ii) cos = θ cos θ = x GE. cos3 θ = x 4 cos θ 3 cos θ = x 4x - 3x = x 4( x - x )= 0 x( x - 1) = 0 x = 0,1, If = + β and - β ) = then + = a) 1 + a b) a + b c) 1 + ab d) 1+ b Ans: c. Solution: α - β ) = 1 b α - β = cos 1 b ) = sin sin (α - β) = b Now sin α + cos β = sin α + 1 sin β 1 + sin α sin β = 1 + sin (α + β) sin (α - β) = 1 + a b If + then x satisfies a) 2x + 3x + 1 =0 b) 2x - 3x = 0 c) 2x + x - 1 =0 d) 2x + x + 1 =0 Ans: b Solution: ( x= 0 satisfies GE and b also. Hence ans b) Or sin + cos 1 sin sin + cos 1 - sin cos 1-2 sin = -2 θ (sin θ = x) 1 x = cos (-2 θ ) = cos 2 θ = 1 2 sin 2 θ 1 x = 1 2x x = 2x 2x - x = 0 x = 0 or x = x = 0 is the solution ( x = does not satisfies the equation )

3 7. If sec -1 x = cosec -1 y then sin -1 ( ) + sin-1 ( ) = a) Π b) π / 2 c) - π /2 d) - π Ans: b. Solution: Given sec -1 x = cosec -1 y cos ) = sin ) sin -1 ( ) + sin-1 ( ) = sin-1 ( ) + cos-1 ( ) =. 8. If tan ax tan bx = 0 ( a b) then the values of x form a series in a) AP b) G P c) H P d) AGP. Ans: a. Solution : tan ax = tan bx ax = n π + bx ax bx = n π x ( a b) = n π x =. put n = 1,2, x=, 9. If ( ) + ( ) = ( ) then x = etc. which are in AP. a) 0 b) c) d) π / 2. Ans: C Solution: w.k.t sin x )+ sin ( y ) = sin ( x1 + y 1 ) sin ( ) + sin ( ) = sin ( 1 )+ 1 ) ) = sin ( ( )/ 9 ) ) x =( )/ 9 Ans c 10. The value of = a) b) c) d). Ans: c Solution: GE = π + tan ( ) -. cot = π + tan ( ) - cot = π - tan ( ) - cot = π [tan ( ) + cot ] = π - = Ans c

4 11. Two angles of a triangle are and, then the third angle is a) b) c) d). Ans: b. Solution: A + B + C = Π where A = cot 2 = tan B= cot 3 = tan. A+ B = tan + tan = tan.. ] = tan 1 ] = C = π - ( A + B) = π - = a) :. : cos sin x cos cos 1 x 1 x sin cos x sin sin 1 x 1 x GE sin 1 x cos 1 x cos x sin x π 2. or Put x 0 then GE sin cos 0 cos sin sin 1 cos 1 π 2. sin If - = then the values of x are a) 0 or ½ b) 1 or 1/3 c) -1 or -1/3 d) -1,1/2 Ans: a Solution type 1: Inspection method: GE is satisfied by a) type 2: GE = cos x sin x = sin 1 x = sin x - sin x = sin 1 x sin 1 x = 2 sin x ( 1 x ) = sin 2 sin x ) = cos 2 sin x ) = 1 2 sin ( sin x) = 1 2x 1 x = 1 2x 2x x 2x x = 0 x ( 2x 1) = 0 x= 0, ½ ----

5 14. If + = then x = a) ± 3 b) 1 c) d) 0 Ans: b. Solution. Inspection method: ± 3 is not a solution since cos 3 is not defined. GE is satisfied by x = The value of + + = a) 0 b) cot 26 c) cot 1 d) cot 1 Ans: a. Solution: w.k.t cot a - cot b = cot cot 21 = cot. = cot 5 - cot 4 Similarly cot 13 = cot 4 - cot 3 And cot 8 = cot 3 - cot 5 GE = cot 5 - cot 4 + cot 4 - cot 3 + cot 3 - cot 5 = If +. = for 0< < then x = a) 1 b) 3) 0 d) Ans: a) Solution: clearly when x = 1 GE = ans: a) Or x = x = = x (2 x x ( 2 + x ) x = 0, 1. But x The value of 2 = a) b) c) d) Ans: b. searching method. put x = 1 then GE = 2tan 2-1] = 2 =. Put x = 1 in choices, Hence cot 1 = tan 1 = b Put x = -1 then GE = 2tan 2 - tan (π ) ] = = 2tan ] = - 2tan 2-1 ] = -2 ( ) = Hence answer must be either a or

6 Put x= -1 in a and b Then cot 1 = π = b tan 1 ) =. Hence answer is b If 2 =, then x is in a) [-1, 1 ] b) [-, 1] c) [- ] d) [ 0, 1]. Ans: c. Solution w.k. t. the range of RHS is [ 2 sin x sin x sin The solution set of the equation = 2 is a) { 1, 2} b) { -1, 2} c) {-1, 1, 0} d) {1, ½, 0} Ans: c) Solution : clearly is not defined. reject a) and b). consider d) = but =. = 2 hence reject d) Only possibility is ans c. or = 2 = x = x( ) = 2x x - = 0 x( 1 x ) = 0 x = 0, ±1 20. If in a triangle ABC, C is 90 0, then + a) b) c) Ans: c) d) = Solution: ABC is a right angled triangle. Put a= 3, b= 4 and c= 5. Then C= 90 Then tan + tan = tan + tan = tan + tan = = tan + tan = where m = 1. Ans: c.

7 21. The value of tan[ ) + )] = a) a b) c) b d) Ans: b). Solution Inspection method. Step1. Put a = 1, b= 0 Then GE = tan [tan 1)] = 1. When we put a=1, b= 0 in choices answer is either a or b Step2. a=0, b= 1 Then GE = tan [tan 1)+ tan 1) ] = tan [ ] = When we put a=0, b= 1 in choices Ans b) ( 1/a = 1/0 = ) If,,...a n is an AP with common difference d, then tan { } = a) b) c) Ans : b ) Solution: Given,,...a n are in AP - a 1 = a 3 a 2 =... a n - a n-1 = d d) Consider tan + tan tan = + tan tan = tan a - tan a + tan a - tan a tan a - tan a = tan a - tan a = tan = = tan =tan GE: tan tan ) = Hence answer is b.

8 23. If + = then x = a) 0 b) 1 c) 2-1 d) 1 Ans: d). Solution: Inspection method: Clearly x = o is not a solution since tan 0 =0 And cot 0 = LHS = When x= 1 LHS of GE = X = I is not a solution When x= 2-1, LHS of GE = is not a solution. x = -1 is only a solution If + + =, then X 1 x = a xyz b) 2xyz c) 2( x+ y + z) d) x y z Ans b Solution: It is a standard result. Or Inspection method. Step 1. put x= y = 1 and z = 0. Then sin x = π and choice b) and d) matches with this value. Step 2. Put x = and z = 1. Then sin x = π and choice b) matches with this value b is the answer If tan( x + y ) = 33 and x = then y = a) b) tan 30 c) tan d) Ans: d) tan Solution: x + y = tan 33 y =tan 33 - tan 3 = tan. =tan tan answer d)

9 26. 2 with x = a) sin 2x b) cos 2x c) cos x d) tan 1 x Ans: c Solution : put x = 1 then GE : When x = 1, a) and b) are not defined due to & c) = 0 and d) =. Hence Ans is c. 27. The general solution of sin5x = k where k is a real root of x - 1 = 0 is given by a) x = + 1 b x = + 1 (c) x = + 1 (d) x = n π + 1 Ans (a). Solution: Consider 2x - x +2x - 1 = 0 x (2x -1) +1 ( 2x 1) = 0 x +1 ) ( 2x 1) = 0 Since x is real x = ½. sin 5x = k = ½ = sin ( ) α = 5x = n π + 1 α = n 1 x = + 1 Ans (a) 28. If 5cos 2 θ = 0, θε (- π, π ),then θ = a) ( b), cos c) cos (d), π - cos Ans: (d ). Solution: GE = 5cos 2 θ + 2 cos + 1 = 0 5( 2 cos θ -1) + ( 1 + cos θ ) + 1 =0 10 x + x - 3 =0 where x = cos θ 10 x + 6x - 5x - 3 =0 2x ( 5x + 3 ) -1 ( 5x + 3 ) =0 x =, cos θ = ½ = cos, and cos θ = = cos( π - cos -1 (3/5)) Solution is, π - cos-1 (3/5)).

10 29. If The general solution of = 3 is given by θ = a) 2n π ± (b) n π ± (c). 2n π ± (b) n π ± Ans: (d) Solution: GE = = 3 tan θ = 3 tan θ =± 3 = tan( ± ) θ = n π ± If Sec x cos5x + 1 =0 where 0<x < 2 π, then x is equal to : a), b) c) d) none of these Ans: c Solution: GE : +1 = 0 cos5x + cosx = 0 2 cos 3x cos 2x =0 Cos 3x = 0 or cos2x =0 3x = or 2x = or X= or or or x = or inspection method. 31. The solution of the equation 2x = 1+ x is a) x = ( 2n + 1 ), n Є Z (b) x = n π, n Є Z.(C) x= ( 2n + 1 ), n Є Z (d) no solution. Ans: d Solution:GE: sin 2x = 1+ cos x Here cos x 0 The max value of LHS is 1 and minimum Vaue of RHS is 1. This is possible only when cos x = 0 and sin 2x = 1 x = and 2x = X =.This is not possible. Hence solution does not exists.

11 32. The most general value of θ satisfying the equation + tan θ - 1) 2 = 0 are given by a) n π ± b) n π + ( -1) n c). 2n π + (d) 2n π + Ans: c. Solution: a b = 0 a = 0 and b =0 1 2 sin θ = 0 and 3 tan θ - 1 = 0 sin θ = - ½ and tan θ = G.S. is θ = m π + ( -1) m and θ = mπ + only when m is odd m = 2n + 1 G.S. is θ = ( 2n + 1)π = 2n π The most general solution of θ satisfying Tan θ + tan( + θ ) = 2 is / are a) n π ±, n Є Z. b) 2n π +, n Є Z.c) 2n π ±, n Є Z d) ) 2n π +( -1) n, n Є Z. Both holds good Ans: a Solution: GE: Tan θ + tan( + θ ) = 2 Tan θ + tan 135 θ = 2 Tan θ + = 2 Tan θ + tan θ tan θ = tan θ tan θ = 3 tan θ = ± 3 θ = n π ±, n Є I The general solution of x for which cos2x,, and sin 2x are in Ap, are given by a) n π, n π + b) n π, n π + c) n π +, d) none of these. Ans: b. Solution: a,b,c are in AP a + c = 2b Cos2x + sin 2x = 1 Sin2x = 1 cos2x = 2 sin 2 x 2 sinx cos x - 2 sin 2 x = 0 2 sinx( cos x sinx) =0 sinx = o or cosx = sinx

12 sinx = 0 or tanx = 1 X = n π or x = n π +, n Є Z. 35. If sec θ + tan θ =1 then the general solution of θ= a) n π + b) 2n π + c) 2n π - d) 2n π ± Ans : c. GE : + = 1 cos θ sin θ = 2 cos( θ + ) = cos( 0 ) G.S. is θ + = 2 n π θ = 2 n π The equation sin cos has a) one solution b) two solutions c) infinite solutions d) no solution. Ans: d GE: sin3x = -2 < - 1. Hence solution does not exists The general solution of ( + ) = 2 is a) x = n π b) x = ( 4n + 1) c) x = ( 4n + 1) d) n π +. Ans: b. Solution clearly x = satisfies the GE If π x Π, π y Π and cos x + cosy = 2 then general solution is x = a) 2 n π + y b) 2 n π - y c) n π + y d) n π + ( -1) n y. Ans a. Solution : the Max. value of cosx is 1. Hence cos x + cosy = 2 cosx = 1 and cosy =1 x = 0 and y = 0 hence x y = 0 Hence cos( x y) = cos 0 X y = 2 n π x = 2 n π + y

13 39. The equation 3 x + 10cosx 6 =0 is satisfied if a) x = n π ± cos b) x = 2n π ± cos c) x = n π ± cos b) x = 2n π ± cos Ans: b. Solution GE.: 3( 1 - cos x ) + 10cosx 6 =0 3 3t + 10 t - 6 =0 where t = cosx 3t - 10 t +3 =0 3t - 9t - t +3 =0 3t( t 3 ) -1 ( t 3) =0 ( 3t -1) (t-3)=0 cosx = t = 3 > 1 No solution, Cosx = 1/3 = cos α where α = cos X = 2n π ± cos i.e. b). 40. If tan2x = tan, then the value of x = a) b) c) d) None of these Ans: a) Solution: GE: tan2x = tan 2x = n π + 2x - nπ x 2 = 0 X = 41. If the equation cos3x x + sin3x x= 0., then x = a) ( 2n+1) b) ( 2n - 1) c) d) n π,. Ans: a:) Solution: put n = 0 in answers a,b,c and d, Substitute x=0, x=, x=. GE is not satisfied when x =0 Hence c and d are not correct answers. GE is not satisfied when x = answer. Hence a is the answer. Or. Hence b is not the correct

14 cos3xcos x + sin3x sin x= 0. cos3x [ ( cos3x + 3 cosx )] + sin3x[ ( 3sinx - sin3x)] =0 ( cos 3x - sin 3x ) +3 ( cos3x cosx + sin3x sinx )} =0 {cos6x + 3 cos2x} =0 2x = A {cos3a + 3 cosa} =0 cos A0 cos 2x 0 cos2x = 0 2x = ( 2n + 1) x = ( 2n + 1) 42. If x and = 1, then all solutions of x are given by a) 2n π + b) ( 2n + 1) π - c) 2n π + 1 d) None of these. Ans : d. Solution: Since x, cos x 0,1,-1. Hence only possibility is sin x 3 sinx 2 = 0 sin x 2 sinx sinx 2 0 ( sinx - 1 ) ( sinx 2) =0 Sin x = 1 or 2 which is not possible as x and 2 > 1 Hence d is the answer. 43. If 1 + sin x + x + x +... = with 0<x < π and x, then x = a) b) c) Ans d. or d) Solution : put sinx = r then GE: 1 + r + r +... = ( in GP.) or With < 1 since 0<x < π and x. S = = = sinx = 1 sinx = x =

15 sinx = 1 - = = x = 60 or 120 Ans: d The general solution of of = cos2x 1 is a) 2n π b) c) n π d) (2n + 1) π Ans: c Solution: when n=1 a) π c) 2 π d is 3 π b) Among these GE is not satisfied by b) b is not the correct answer. Since GE is satisfied for π, 2π, 3 π also. General solution is θ = n π. Or tan x = cos2x 1 = - ( 1 cos2x) = - 2sin x sin x = - 2sin x cos x sin x ( 1 + 2cos x ) = 0 sin x = 0 sinx = 0 x= n π where n Є Z Cot θ =sin2 θ ( θ n π ),if θ = a), b), c) only d) only Ans b) Solution : when θ =, in GE LHS = RHS = 1. GE is satisfied by θ = also. and solution θ =,. Or GE = 2 sin θ cos θ cos θ = 2 sin θ cos θ cos θ ( 1-2 sin θ ) = 0 is not a Cos θ =0 θ = sin θ = ½ sin θ = ± θ = ±

16 46. If sin( cotθ ) =cos( tanθ) then the value of θ = a)n π + b ) 2n π ± c) n π - d) 2n π ± Ans: a) Solution: we know that sin = cos π cotθ = π tanθ cotθ = tanθ tan θ = 1 θ = n π If tan θ + 3 cot θ = 5 sec θ then θ = a) n π + ( -1) n, nє Z. b) n π + ( -1) n, nє Z c) n π + ( -1) n+ 1, nє Z or n π + ( -1) n, nє Z d) n π + ( -1) n, nє Z or n π + ( -1) n, nє Z Ans: b). Solution. GE: +3 sin θ + 3 cos θ = 5 sin θ cos θ = 5sin θ which is satisfied for x = only. answer is b) If tanx + tan4x + tan7x = tanx tan4x tan7x then x = a) n π / 3 b) n π / 4 c) n π / 6 d) n π / 12 Ans d). Solution : w. k.t if tan x + tany + tanz = tanx tany tanz then ] tan( x + y + z ) = 0. tan12x = 0 12x = n π x = n π / The general solution of sinx + sin7x = sin4x in ( 0, ) are a), b), c), d), Ans d) Solution: GE : sin7x + sin x sin4x =0 2 sin4x cos 3x sin 4x =0 sin4x( 2 cos3x - 1) =0 sin4x =0 4x = n π or x = n π / 4 = π / 4 in ( 0, ) cos 3x = = cos ( ) in ( 0, ) 3x = x = x =, Ans d

17 50. The number of solutions of cosx =, 0x 3 π is a) 3 b) 2 c) 4 d) 5 Ans: a. Solution: clearly 1 0 cosx = 1 + sinx ( = x if x 0 ) cos x sin x = 1 By inspection x = 0, 2π, 3 π /2 are 3 solutions in [0,3π] Ans a The set of values of x for which a) φ b) { n π +, n Є Z } c) Ans a. Solution: Clearly tan x = 1 = tan ( ) = 1 is d) { 2n π +, n Є Z } X = n π +, n Є Z. But for no values of x, sin2x is not defined, so that the equation has no solution. 52. The general solution of cos7 θ cos 5 θ = cos3θ cosθ is a), b), c), d ), Ans c. Solution : GE: cos7 θ cos 5 θ = cos3θ cosθ ( cos12 θ + cos2 θ ) = ( cos 4 θ + cos2 θ ) cos12 θ cos 4 θ = 0-2 sin 8θ sin 4θ =0 8θ = n or 4θ = n θ = Ans c If sec 2 x + + cosec 2 x = 4, then the value of x is a) b) c) d) Ans d. Clearly by inspection method d) is the answer ,

18 54. The equation 2 sin θ cos θ = x 2 + has a) one real solution b) no solution c) two real solutions d) θ = n π. ans b) Solution : GE : sin 2 θ = x 2 +. clearly sin 2 θ > 0. If x 1 solution does not exists. If 0<x< 1 then x < 1 but >1 hence x 2 + > 1 Solution does not exists. no solution 55. If A and B are acute angles such that sina = sin 2 B and 2 cos 2 A = 3 cos 2 B then A is d) a) b) c) Solution : Clearly by inspection method A=. Since when A=, B = from sina = sin 2 B. These values satisfies 2 cos 2 A = 3 cos 2 B also. a = is the ans Let n be a positive integer such that sin + cos =,then a) n = 4 b) n= 1,2,3,4,... c) n = 2 d) n = 6 Ans d. Solution: clearly by inspection n = 6. Or sin + cos squaring sin cos = sin = - 1 = which is true when n = 6. sin = n =6 only. 57. If sin 40 0 = k and cosx = 1 2 then the value of x in ( 0 0, ) are a) 40 o and 140 o b) 80 o and 280 o c) 40 o and 220 o d) 80 o and 260 o Ans: b. Solution : Now cosx = 1 2 sin = cos80 0. x = 80 0 and = x = 80 0, in ( 0 0, ) =

19 58. If 3 cos 2 x - 2 cos x sinx - 3 sin 2 x = 0 then x = a) + b) + c) d) n π + Ans: a) Solution : GE: 3 cos2x - 3 sin2x =0 3 cos2x = 3 sin2x = 3 tan2x = x = n π + x = The most general solution of + =0 a) 2n π +, n ЄZ, b) n π +, n ЄZ c) 2n π -, n ЄZ d) n π -, n ЄZ Ans: b. Solution: GE: log tanx = - log cotx log tanx = - log = log tanx log tanx = log tanx sinx = cosx Tanx = 1 x = n π +, n ЄZ ans :b The general solution of 3 tan( θ 15 o )= tan ( θ + 15 o ) is a) θ = ± b) n ± c) + ( -1) n d) 2n - Ans: c Solution: 3 tan( θ 15 o )= tan ( θ + 15 o ) 3 = 3 sin θ 15 cos θ 15 = sin θ 15 cos θ 15 2 sin θ 15 cos θ 15 + sin ( ) =0 sin2 θ + sin ( ) + sin ( ) =0 Sin 2 θ = 1 2 θ = n π + ( -1) n θ = ( -1) n

20 61. The most general solution of tan θ +1 = 0 & secθ - 2 =0 is a) 2n π - c) n π + ( -1) n Ans b) Solution: Given b) 2n π + d) 2n π + tan θ = quadrant take θ = 2 π = general solution is θ = 2n π + and cos θ = Ans b. θ in IV 62. If cosx + cosy = 1 and cosxcosy = ¼ then the general solutions are a) x = 2n π ±, y = 2k π ± b) 2n π ±, y = 2k π ± c) x = 2n π ±, y = 2k π ± b) n π ±, y = k π ± Ans: b. Solution: clearly by inspection method x =, y= is a solution. Hence ans is b). Or Cosx cosy = cosx cosy 4 cosxcosy = 1 4 =0 Now cosx + cosy = 1 and cosx - cosy = 0 cosx = ½ and cosy = ½ x = 2n π ±, y = 2k π ± ans : b = a b) - c) d) Ans : c Solution: put x= 0 then GE : In choices only a and c results in Hence answer is either a or c.. Put x = then GE: tan = tan 3= In choices a reduces to 15 0 and c reduces to Hence c is the answer.

21 Tan[ + cos-1 ( ) ] + Tan[ - cos-1 ( ) ] with x 0 a) 2x b) c) 2x d) 2 1 x Ans: b) Solution : put x = 1 in GE: = 2 reject d. Put x = in GE: tan( ) + tan ( ) = tan ( 750 ) + tan 15 0 = = 4 In choices b) gives 4. hence b is the correct answer If sin -1 ( ) + ) =, then x = a) 4 b) 5 c ) 1 d) 3 Ans: d. Solution: cosec ) = sin-1 ( ) GE : sin -1 ( ) + sin-1 ( ) = sin -1 ( ) = cos-1 ( ) clearly x = 3. sin -1 ( ) = cos-1 ( ) The value of cos( 2 + ) at x = 1/5 is a) b) c) d) 2 6 Ans: b Solution: cos( 2cos x + sin x ) = cos ( + cos x ) = - sin (cos x ) = - sin (sin 1 x ) = - 1 x At x = 1/5 ans is - 1 = - = The general solution of cosecx + cotx = is a) x = 2n π ± b) x = + - c) x = - d) x = 2n π ± - Ans: d. Solution: GE: cosecx + cotx = cosx = 3 sinx cosx + 3 sinx = - 1 cosx + cos( x + ) = cos G.S. is x = 2n π ± - ans :d..

22 68. If α, β and γ are the roots of the equation x 3 + m x 2 + 3x + m = 0, then the general solution of + + = a) ( 2n + 1) b) n π c) d) depend upon the value of x. Ans: b Solution : consider x 3 + m x 2 + 3x + m = 0 α = -b/a = -m, α = c/a = 3 ; α β γ = -d/a = -m Now =tan tan α + tan β + tan γ = tan = tan -1 (0) =0. G.S. is tan α +tan β +tan γ = n.where n Є Z. Ans b 69. The equation 3 cosx + 4 sinx = 6 has a) finite solution b) infinite solution c) one solution d) no solution. Ans: d Here r = > 1 where a= 3, b= 4 c = 6. Hence no solution. 70. The value of x satisfying the equation sinx + is given by a) 10 0 b) 30 0 c) 45 0 d) 60 0 = Ans: d Solution : Clearly by inspection x = 60 0 satisfies the equation. because sin = + = 71. If log 5 (1 + sinx) + log 5 (1 - sinx) = 0 then x in ( 0, ) is a) b) 0 c) d No value Ans d Solution: Clearly If log 5 [ (1 + sinx)( 1 sinx)] =0 1 sin 2 x = 0 cos 2 x =1 cosx = ± 1 x = 0, 0, ) no value.

23 72. If y = cosx and y = sin 5x then x = a) b) c) d) Ans: c Solution: clearly sin5x = cosx sin5x = sin ( - x) 5x = - x 6x = x = ans C 73. The value of ) ) + ) ) = a) Ans: d : b) c) = 2. d) 0 cos cos ) ) = cos cos 2π ) ) = sin sin ) = sin sin2π ) = - GE: = 0 Ans: d 74. If θ = )), then one of the possible value of θ is a) b) c) d) Ans: a) Solution: = θ = sin sin 600 = sin sin 120 = sin sin ) = sin sin 60 ) = 60 = 75. The value of sin( 2. = a) 0.96 b) 0.86 c) 0.94 d) Ans a) Solution: 0.8 = sin( 2 sin 0.8 = sin ( 2 θ ) where θ = sin = 2 sin θ cos θ = 2.. = = Ans a)

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

Matrices and Determinants

Matrices 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 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

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

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

Example Sheet 3 Solutions

Example 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 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

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

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

Homework 3 Solutions

Homework 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 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

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

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

TRIGONOMETRIC FUNCTIONS

TRIGONOMETRIC FUNCTIONS Chapter TRIGONOMETRIC FUNCTIONS. Overview.. The word trigonometry is derived from the Greek words trigon and metron which means measuring the sides of a triangle. An angle is the amount of rotation of

Διαβάστε περισσότερα

Finite Field Problems: Solutions

Finite 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 περισσότερα

Answers - 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 =

Answers - 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 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

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

Section 7.6 Double and Half Angle Formulas

Section 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 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

COMPLEX NUMBERS. 1. A number of the form.

COMPLEX NUMBERS. 1. A number of the form. COMPLEX NUMBERS SYNOPSIS 1. A number of the form. z = x + iy is said to be complex number x,yєr and i= -1 imaginary number. 2. i 4n =1, n is an integer. 3. In z= x +iy, x is called real part and y is called

Διαβάστε περισσότερα

2 Composition. Invertible Mappings

2 Composition. Invertible Mappings Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,

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

IIT JEE (2013) (Trigonomtery 1) Solutions

IIT JEE (2013) (Trigonomtery 1) Solutions L.K. Gupta (Mathematic Classes) www.pioeermathematics.com MOBILE: 985577, 677 (+) PAPER B IIT JEE (0) (Trigoomtery ) Solutios TOWARDS IIT JEE IS NOT A JOURNEY, IT S A BATTLE, ONLY THE TOUGHEST WILL SURVIVE

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

EE512: Error Control Coding

EE512: 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 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

MathCity.org Merging man and maths

MathCity.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 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

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

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Exercises 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 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

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

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

ST5224: Advanced Statistical Theory II

ST5224: 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 περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL 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 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

The Simply Typed Lambda Calculus

The Simply Typed Lambda Calculus Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and

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

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

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

L.K.Gupta (Mathematic Classes) www.pioeermathematics.com MOBILE: 985577, 4677 + {JEE Mai 04} Sept 0 Name: Batch (Day) Phoe No. IT IS NOT ENOUGH TO HAVE A GOOD MIND, THE MAIN THING IS TO USE IT WELL Marks:

Διαβάστε περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 Autoregressive Moving Average Model ARMA(1,1) 84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this

Διαβάστε περισσότερα

Second Order RLC Filters

Second 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 περισσότερα

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

k 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 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

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

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other Test Constructions: Likelihood Ratio & Bayes Tests Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :

Διαβάστε περισσότερα

6.3 Forecasting ARMA processes

6.3 Forecasting ARMA processes 122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear

Διαβάστε περισσότερα

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required) Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts

Διαβάστε περισσότερα

Chapter 6 BLM Answers

Chapter 6 BLM Answers Chapter 6 BLM Answers BLM 6 Chapter 6 Prerequisite Skills. a) i) II ii) IV iii) III i) 5 ii) 7 iii) 7. a) 0, c) 88.,.6, 59.6 d). a) 5 + 60 n; 7 + n, c). rad + n rad; 7 9,. a) 5 6 c) 69. d) 0.88 5. a) negative

Διαβάστε περισσότερα

Statistical Inference I Locally most powerful tests

Statistical Inference I Locally most powerful tests Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided

Διαβάστε περισσότερα

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

DESIGN 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 περισσότερα

derivation of the Laplacian from rectangular to spherical coordinates

derivation of the Laplacian from rectangular to spherical coordinates derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used

Διαβάστε περισσότερα

Differentiation exercise show differential equation

Differentiation 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 περισσότερα

Solution Series 9. i=1 x i and i=1 x i.

Solution 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 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

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

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

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

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that

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

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal

Διαβάστε περισσότερα

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

9.09. # 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 περισσότερα

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Απόκριση 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 περισσότερα

Problem 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.

Problem 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 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

F-TF Sum and Difference angle

F-TF Sum and Difference angle F-TF Sum and Difference angle formulas Alignments to Content Standards: F-TF.C.9 Task In this task, you will show how all of the sum and difference angle formulas can be derived from a single formula when

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

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

Every set of first-order formulas is equivalent to an independent set

Every set of first-order formulas is equivalent to an independent set Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent

Διαβάστε περισσότερα

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8  questions or comments to Dan Fetter 1 Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test

Διαβάστε περισσότερα

Fractional Colorings and Zykov Products of graphs

Fractional Colorings and Zykov Products of graphs Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is

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

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

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

Srednicki Chapter 55

Srednicki Chapter 55 Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third

Διαβάστε περισσότερα

( ) 2 and compare to M.

( ) 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 περισσότερα

3.4. Click here for solutions. Click here for answers. CURVE SKETCHING. y cos x sin x. x 1 x 2. x 2 x 3 4 y 1 x 2. x 5 2

3.4. Click here for solutions. Click here for answers. CURVE SKETCHING. y cos x sin x. x 1 x 2. x 2 x 3 4 y 1 x 2. x 5 2 SECTION. CURVE SKETCHING. CURVE SKETCHING A Click here for answers. S Click here for solutions. 9. Use the guidelines of this section to sketch the curve. cos sin. 5. 6 8 7 0. cot, 0.. 9. cos sin. sin

Διαβάστε περισσότερα

( y) Partial Differential Equations

( y) Partial Differential Equations Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS 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 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

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. Dirac Equation. Hamiltonian. Dirac Eq. 6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2

Διαβάστε περισσότερα

Strain gauge and rosettes

Strain 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 περισσότερα

Problem Set 3: Solutions

Problem Set 3: Solutions CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C

Διαβάστε περισσότερα

EE1. Solutions of Problems 4. : a) f(x) = x 2 +x. = (x+ǫ)2 +(x+ǫ) (x 2 +x) ǫ

EE1. 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 περισσότερα

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Partial Differential Equations in Biology The boundary element method. March 26, 2013 The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS 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 περισσότερα

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p) Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok

Διαβάστε περισσότερα

7. TRIGONOMETRIC RATIOS, IDENTITIES AND EQUATIONS 1. INTRODUCTION 2. TRIGONOMETRIC FUNCTIONS (CIRCULAR FUNCTIONS)

7. TRIGONOMETRIC RATIOS, IDENTITIES AND EQUATIONS 1. INTRODUCTION 2. TRIGONOMETRIC FUNCTIONS (CIRCULAR FUNCTIONS) 7. TRIGONOMETRIC RATIOS, IDENTITIES AND EQUATIONS. INTRODUCTION The equations involving trigonometric functions of unknown angles are known as Trigonometric equations e.g. cos 0,cos cos,sin + sin cos sin..

Διαβάστε περισσότερα

Uniform Convergence of Fourier Series Michael Taylor

Uniform Convergence of Fourier Series Michael Taylor Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula

Διαβάστε περισσότερα

Paper Reference. Paper Reference(s) 6665/01 Edexcel GCE Core Mathematics C3 Advanced. Thursday 11 June 2009 Morning Time: 1 hour 30 minutes

Paper Reference. Paper Reference(s) 6665/01 Edexcel GCE Core Mathematics C3 Advanced. Thursday 11 June 2009 Morning Time: 1 hour 30 minutes Centre No. Candidate No. Paper Reference(s) 6665/01 Edexcel GCE Core Mathematics C3 Advanced Thursday 11 June 2009 Morning Time: 1 hour 30 minutes Materials required for examination Mathematical Formulae

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

*H31123A0228* 1. (a) Find the value of at the point where x = 2 on the curve with equation. y = x 2 (5x 1). (6)

*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 περισσότερα

ω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω

ω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω 0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΕΤΑΙΡΕΙΑ IΔ ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΟΛΥΜΠΙΑΔΑ 2013 21 ΑΠΡΙΛΙΟΥ 2013 Β & Γ ΛΥΚΕΙΟΥ. www.cms.org.cy

ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΕΤΑΙΡΕΙΑ IΔ ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΟΛΥΜΠΙΑΔΑ 2013 21 ΑΠΡΙΛΙΟΥ 2013 Β & Γ ΛΥΚΕΙΟΥ. www.cms.org.cy ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΕΤΑΙΡΕΙΑ IΔ ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΟΛΥΜΠΙΑΔΑ 2013 21 ΑΠΡΙΛΙΟΥ 2013 Β & Γ ΛΥΚΕΙΟΥ www.cms.org.cy ΘΕΜΑΤΑ ΣΤΑ ΕΛΛΗΝΙΚΑ ΚΑΙ ΑΓΓΛΙΚΑ PAPERS IN BOTH GREEK AND ENGLISH ΚΥΠΡΙΑΚΗ ΜΑΘΗΜΑΤΙΚΗ ΟΛΥΜΠΙΑΔΑ

Διαβάστε περισσότερα

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all

Διαβάστε περισσότερα

DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation

DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation DiracDelta Notations Traditional name Dirac delta function Traditional notation x Mathematica StandardForm notation DiracDeltax Primary definition 4.03.02.000.0 x Π lim ε ; x ε0 x 2 2 ε Specific values

Διαβάστε περισσότερα