• 検索結果がありません。

2 sin cos θ θ = cos θ

N/A
N/A
Protected

Academic year: 2021

シェア "2 sin cos θ θ = cos θ"

Copied!
2
0
0

読み込み中.... (全文を見る)

全文

(1)

0

θ < 2 π

のとき,次の方程式を解け。

(1)

sin 2 θ = cos θ

2 sin cos θ θ = cos θ

cos (2 sin θ θ − = 1) 0

よって

cos θ = 0

…① または

1

sin θ = 2

…②

①のとき

3

2 , 2

θ = π π

, ②のとき

5 6 , 6 θ = π π

したがって

5 3

, , ,

6 2 6 2

π π

θ = π π

〔別解〕

sin 2 sin 2 θ =   π − θ  

n ∈ 

とし,一般角で考えて

2 2

2

n

θ =   π − θ   + π

より

2

6 3

π

n

π θ = +

2 2

2

n

θ π = −   π − θ   + π

より

θ = π 2 +

n

π

この中で,

0

θ < 2 π

にあたるものは

5 3

, , ,

6 2 6 2

π π

θ = π π

(2)

cos 2 θ + cos θ + = 1 0

2 cos

2

θ − + 1 cos θ + = 1 0

cos (2 cos θ θ + = 1) 0

よって

cos θ = 0

…① または

1

cos θ = − 2

…②

①のとき

θ = 0

, ②のとき

2 4 3 , 3 θ = π π

したがって

2 4

0, ,

3 3

θ = π π

sin α = sin β

のとき,単純に

α β =

とすることはできません。正しくは

sin α = sin β

α β = + 2n π

n ∈ 

)または

α π β = − + 2n π

n ∈ 

です。

86.三角関数を含む方程式③

(1)

5 3

, , ,

6 2 6 2

π π

θ = π π

(2)

2 4

0, ,

3 3

θ = π π

(3)

3 5 3 7

, , , , ,

4 2 4 4 2 4

π π

θ = π π π π

(4)

3 7 11 15

0, , , , ,

8 8 8 8

θ = π π π π π

(2)

(3)

cos θ + cos 3 θ = 0

cos θ − 3cos θ + 4 cos

3

θ = 0

2 cos

3

θ − cos θ = 0

cos θ ( 2 cos θ + 1 )( 2 cos θ − = 1 ) 0

よって

cos θ = 0

…① または

1

cos θ = 2

…② または

1

cos θ = − 2

…③

①のとき

3

2 , 2

θ = π π

, ②のとき

7 4 , 4

θ = π π

, ③のとき

3 5 4 , 4 θ = π π

したがって

3 5 3 7

, , , , ,

4 2 4 4 2 4

π π

θ = π π π π

(4)

sin 3 θ − sin θ = cos 3 θ − cos θ

3 3 3 3

2 cos sin 2 sin sin

2 2 2 2

θ θ + θ θ − = − θ θ + θ θ −

2 cos 2 sin θ θ = − 2 sin 2 sin θ θ

sin (sin 2 θ θ + cos 2 ) θ = 0

sin 2 sin 2 0

4 θ ⋅   θ + π   =

sin sin 2 0

4 θ   θ + π   =

よって

sin θ = 0

…① または

sin 2 0 4 θ π

 +  =

 

 

…②

①のとき

θ = 0, π

②のとき

17

4 2 4 4

π

θ + π < π

であるから

2 , 2 , 3 , 4 4

θ + π = π π π π

3 7 11 15

, , ,

8 8 8 8

θ = π π π π

したがって

3 7 11 15

0, , , , ,

8 8 8 8

θ = π π π π π

参照

関連したドキュメント

In the present work, which is self-contained, we study the general case of a reward given by an admissible family φ = (φ(θ), θ ∈ T 0 ) of non negative random variables, and we solve

The Goal of Hodge theaters: Roughly speaking, Hodge theater (at least, the ´ etale part) is a virtual “GMS” for an arbitrary elliptic curve over a number field which manages.. Θ

Abstract: In this paper, we proved a rigidity theorem of the Hodge metric for concave horizontal slices and a local rigidity theorem for the monodromy representation.. I

As an application of this result, the asymptotic stability of stochastic numerical methods, such as partially drift-implicit θ-methods with variable step sizes for ordinary

If there is a NE path from 0 to (r, θ ) with less than C r/2 bad edges among these C r closed edges, note that each good edge costs at least passage time δ, so the passage time of

To derive a weak formulation of (1.1)–(1.8), we first assume that the functions v, p, θ and c are a classical solution of our problem. 33]) and substitute the Neumann boundary

— In this paper, we give a brief survey on the fundamental group of the complement of a plane curve and its Alexander polynomial.. We also introduce the notion of

Key Words: Wiener amalgam spaces, Feichtinger’s algebra, homogeneous Banach spaces, Besov-, Sobolev-, fractional Sobolev spaces, modulation spa- ces, Herz spaces,