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人気のある三角関数 >

tan^2(x)-sin(x)=tan^2(x)sin^2(x)

解

tan^{2} (x) - sin (x) = tan^{2} (x) sin^{2} (x)

解

x = 2 πn, x = π + 2 πn

+1

度

x = 0^{\circ} + 36 0^{\circ} n, x = 18 0^{\circ} + 36 0^{\circ} n

解答ステップ

tan^{2} (x) - sin (x) = tan^{2} (x) sin^{2} (x)

両辺から

tan^{2} (x) sin^{2} (x)

を引く

tan^{2} (x) - sin (x) - tan^{2} (x) sin^{2} (x) = 0

サイン, コサインで表わす

- sin (x) + tan^{2} (x) - sin^{2} (x) tan^{2} (x)

基本的な三角関数の公式を使用する:

tan (x) = \frac{sin ( x )}{cos ( x )}

= - sin (x) + (\frac{sin ( x )}{cos ( x )})^{2} - sin^{2} (x) (\frac{sin ( x )}{cos ( x )})^{2}

簡素化

- sin (x) + (\frac{sin ( x )}{cos ( x )})^{2} - sin^{2} (x) (\frac{sin ( x )}{cos ( x )})^{2} : \frac{- cos ^{2} ( x ) sin ( x ) + sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

- sin (x) + (\frac{sin ( x )}{cos ( x )})^{2} - sin^{2} (x) (\frac{sin ( x )}{cos ( x )})^{2}

(\frac{sin ( x )}{cos ( x )})^{2} = \frac{sin ^{2} ( x )}{cos ^{2} ( x )}

(\frac{sin ( x )}{cos ( x )})^{2}

指数の規則を適用する:

(\frac{a}{b})^{c} = \frac{a ^{c}}{b ^{c}}

= \frac{sin ^{2} ( x )}{cos ^{2} ( x )}

sin^{2} (x) (\frac{sin ( x )}{cos ( x )})^{2} = \frac{sin ^{4} ( x )}{cos ^{2} ( x )}

sin^{2} (x) (\frac{sin ( x )}{cos ( x )})^{2}

(\frac{sin ( x )}{cos ( x )})^{2} = \frac{sin ^{2} ( x )}{cos ^{2} ( x )}

(\frac{sin ( x )}{cos ( x )})^{2}

指数の規則を適用する:

(\frac{a}{b})^{c} = \frac{a ^{c}}{b ^{c}}

= \frac{sin ^{2} ( x )}{cos ^{2} ( x )}

= \frac{sin ^{2} ( x )}{cos ^{2} ( x )} sin^{2} (x)

分数を乗じる:

a \cdot \frac{b}{c} = \frac{a \cdot b}{c}

= \frac{sin ^{2} ( x ) sin ^{2} ( x )}{cos ^{2} ( x )}

sin^{2} (x) sin^{2} (x) = sin^{4} (x)

sin^{2} (x) sin^{2} (x)

指数の規則を適用する:

a^{b} \cdot a^{c} = a^{b + c}

sin^{2} (x) sin^{2} (x) = sin^{2 + 2} (x)

= sin^{2 + 2} (x)

数を足す:

2 + 2 = 4

= sin^{4} (x)

= \frac{sin ^{4} ( x )}{cos ^{2} ( x )}

= - sin (x) + \frac{sin ^{2} ( x )}{cos ^{2} ( x )} - \frac{sin ^{4} ( x )}{cos ^{2} ( x )}

分数を組み合わせる

\frac{sin ^{2} ( x )}{cos ^{2} ( x )} - \frac{sin ^{4} ( x )}{cos ^{2} ( x )} : \frac{sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

規則を適用

\frac{a}{c} \pm \frac{b}{c} = \frac{a \pm b}{c}

= \frac{sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

= - sin (x) + \frac{sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

元を分数に変換する:

sin (x) = \frac{sin ( x ) cos ^{2} ( x )}{cos ^{2} ( x )}

= - \frac{sin ( x ) cos ^{2} ( x )}{cos ^{2} ( x )} + \frac{sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

分母が等しいので, 分数を組み合わせる:

\frac{a}{c} \pm \frac{b}{c} = \frac{a \pm b}{c}

= \frac{- sin ( x ) cos ^{2} ( x ) + sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

= \frac{- cos ^{2} ( x ) sin ( x ) + sin ^{2} ( x ) - sin ^{4} ( x )}{cos ^{2} ( x )}

\frac{sin ^{2} ( x ) - sin ^{4} ( x ) - cos ^{2} ( x ) sin ( x )}{cos ^{2} ( x )} = 0

\frac{f ( x )}{g ( x )} = 0 \Rightarrow f (x) = 0

sin^{2} (x) - sin^{4} (x) - cos^{2} (x) sin (x) = 0

因数

sin^{2} (x) - sin^{4} (x) - cos^{2} (x) sin (x) : sin (x) (sin (x) - sin^{3} (x) - cos^{2} (x))

sin^{2} (x) - sin^{4} (x) - cos^{2} (x) sin (x)

指数の規則を適用する:

a^{b + c} = a^{b} a^{c}

sin^{4} (x) = sin (x) sin^{3} (x), sin^{2} (x) = sin (x) sin (x)

= sin (x) sin (x) - sin (x) sin^{3} (x) - sin (x) cos^{2} (x)

共通項をくくり出す

sin (x)

= sin (x) (sin (x) - sin^{3} (x) - cos^{2} (x))

sin (x) (sin (x) - sin^{3} (x) - cos^{2} (x)) = 0

各部分を別個に解く

sin (x) = 0 or sin (x) - sin^{3} (x) - cos^{2} (x) = 0

sin (x) = 0 : x = 2 πn, x = π + 2 πn

sin (x) = 0

以下の一般解

sin (x) = 0

sin (x)

2 πn

循環を含む周期性テーブル:

x 0 \frac{π}{6} \frac{π}{4} \frac{π}{3} \frac{π}{2} \frac{2 π}{3} \frac{3 π}{4} \frac{5 π}{6} sin (x) 0 \frac{1}{2} \frac{2}{2} \frac{3}{2} 1 \frac{3}{2} \frac{2}{2} \frac{1}{2} x π \frac{7 π}{6} \frac{5 π}{4} \frac{4 π}{3} \frac{3 π}{2} \frac{5 π}{3} \frac{7 π}{4} \frac{11 π}{6} sin (x) 0 - \frac{1}{2} - \frac{2}{2} - \frac{3}{2} - 1 - \frac{3}{2} - \frac{2}{2} - \frac{1}{2}

x = 0 + 2 πn, x = π + 2 πn

x = 0 + 2 πn, x = π + 2 πn

解く

x = 0 + 2 πn : x = 2 πn

x = 0 + 2 πn

0 + 2 πn = 2 πn

x = 2 πn

x = 2 πn, x = π + 2 πn

sin (x) - sin^{3} (x) - cos^{2} (x) = 0 : x = \frac{π}{2} + 2 πn, x = \frac{3 π}{2} + 2 πn

sin (x) - sin^{3} (x) - cos^{2} (x) = 0

三角関数の公式を使用して書き換える

- cos^{2} (x) + sin (x) - sin^{3} (x)

ピタゴラスの公式を使用する:

cos^{2} (x) + sin^{2} (x) = 1

cos^{2} (x) = 1 - sin^{2} (x)

= - (1 - sin^{2} (x)) + sin (x) - sin^{3} (x)

- (1 - sin^{2} (x)) : - 1 + sin^{2} (x)

- (1 - sin^{2} (x))

括弧を分配する

= - (1) - (- sin^{2} (x))

マイナス・プラスの規則を適用する

- (- a) = a, - (a) = - a

= - 1 + sin^{2} (x)

= - 1 + sin^{2} (x) + sin (x) - sin^{3} (x)

- 1 + sin (x) + sin^{2} (x) - sin^{3} (x) = 0

置換で解く

- 1 + sin (x) + sin^{2} (x) - sin^{3} (x) = 0

仮定:

sin (x) = u

- 1 + u + u^{2} - u^{3} = 0

- 1 + u + u^{2} - u^{3} = 0 : u = 1, u = - 1

- 1 + u + u^{2} - u^{3} = 0

標準的な形式で書く

a_{n} x^{n} + \dots + a_{1} x + a_{0} = 0

- u^{3} + u^{2} + u - 1 = 0

因数

- u^{3} + u^{2} + u - 1 : - (u - 1)^{2} (u + 1)

- u^{3} + u^{2} + u - 1

共通項をくくり出す

- 1

= - (u^{3} - u^{2} - u + 1)

因数

u^{3} - u^{2} - u + 1 : (u - 1) (u + 1) (u - 1)

u^{3} - u^{2} - u + 1

= (u^{3} - u^{2}) + (- u + 1)

- 1

を

- u + 1 : - (u - 1)

からくくり出す

- u + 1

共通項をくくり出す

- 1

= - (u - 1)

u^{2}

を

u^{3} - u^{2} : u^{2} (u - 1)

からくくり出す

u^{3} - u^{2}

指数の規則を適用する:

a^{b + c} = a^{b} a^{c}

u^{3} = u u^{2}

= u u^{2} - u^{2}

共通項をくくり出す

u^{2}

= u^{2} (u - 1)

= - (u - 1) + u^{2} (u - 1)

共通項をくくり出す

u - 1

= (u - 1) (u^{2} - 1)

因数

u^{2} - 1 : (u + 1) (u - 1)

u^{2} - 1

1

を書き換え

1^{2}

= u^{2} - 1^{2}

2乗の差の公式を適用する:

x^{2} - y^{2} = (x + y) (x - y)

u^{2} - 1^{2} = (u + 1) (u - 1)

= (u + 1) (u - 1)

= (u - 1) (u + 1) (u - 1)

= - (u - 1) (u + 1) (u - 1)

改良

= - (u - 1)^{2} (u + 1)

- (u - 1)^{2} (u + 1) = 0

零因子の原則を使用:

ab = 0

ならば

a = 0

または

b = 0

u - 1 = 0 or u + 1 = 0

解く

u - 1 = 0 : u = 1

u - 1 = 0

1

を右側に移動します

u - 1 = 0

両辺に

1

を足す

u - 1 + 1 = 0 + 1

簡素化

u = 1

u = 1

解く

u + 1 = 0 : u = - 1

u + 1 = 0

1

を右側に移動します

u + 1 = 0

両辺から

1

を引く

u + 1 - 1 = 0 - 1

簡素化

u = - 1

u = - 1

解答は

u = 1, u = - 1

代用を戻す

u = sin (x)

sin (x) = 1, sin (x) = - 1

sin (x) = 1, sin (x) = - 1

sin (x) = 1 : x = \frac{π}{2} + 2 πn

sin (x) = 1

以下の一般解

sin (x) = 1

sin (x)

2 πn

循環を含む周期性テーブル:

x 0 \frac{π}{6} \frac{π}{4} \frac{π}{3} \frac{π}{2} \frac{2 π}{3} \frac{3 π}{4} \frac{5 π}{6} sin (x) 0 \frac{1}{2} \frac{2}{2} \frac{3}{2} 1 \frac{3}{2} \frac{2}{2} \frac{1}{2} x π \frac{7 π}{6} \frac{5 π}{4} \frac{4 π}{3} \frac{3 π}{2} \frac{5 π}{3} \frac{7 π}{4} \frac{11 π}{6} sin (x) 0 - \frac{1}{2} - \frac{2}{2} - \frac{3}{2} - 1 - \frac{3}{2} - \frac{2}{2} - \frac{1}{2}

x = \frac{π}{2} + 2 πn

x = \frac{π}{2} + 2 πn

sin (x) = - 1 : x = \frac{3 π}{2} + 2 πn

sin (x) = - 1

以下の一般解

sin (x) = - 1

sin (x)

2 πn

循環を含む周期性テーブル:

x 0 \frac{π}{6} \frac{π}{4} \frac{π}{3} \frac{π}{2} \frac{2 π}{3} \frac{3 π}{4} \frac{5 π}{6} sin (x) 0 \frac{1}{2} \frac{2}{2} \frac{3}{2} 1 \frac{3}{2} \frac{2}{2} \frac{1}{2} x π \frac{7 π}{6} \frac{5 π}{4} \frac{4 π}{3} \frac{3 π}{2} \frac{5 π}{3} \frac{7 π}{4} \frac{11 π}{6} sin (x) 0 - \frac{1}{2} - \frac{2}{2} - \frac{3}{2} - 1 - \frac{3}{2} - \frac{2}{2} - \frac{1}{2}

x = \frac{3 π}{2} + 2 πn

x = \frac{3 π}{2} + 2 πn

すべての解を組み合わせる

x = \frac{π}{2} + 2 πn, x = \frac{3 π}{2} + 2 πn

すべての解を組み合わせる

x = 2 πn, x = π + 2 πn, x = \frac{π}{2} + 2 πn, x = \frac{3 π}{2} + 2 πn

equationは以下で未定義のため:

\frac{π}{2} + 2 πn, \frac{3 π}{2} + 2 πn

x = 2 πn, x = π + 2 πn

グラフ

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