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人気のある三角関数 >

cos^2(a)= 3/(5sin(a))

解

cos^{2} (a) = \frac{3}{5 sin ( a )}

解

以下の解はない : a \in R

解答ステップ

cos^{2} (a) = \frac{3}{5 sin ( a )}

両辺から

\frac{3}{5 sin ( a )}

を引く

cos^{2} (a) - \frac{3}{5 sin ( a )} = 0

簡素化

cos^{2} (a) - \frac{3}{5 sin ( a )} : \frac{5 cos ^{2} ( a ) sin ( a ) - 3}{5 sin ( a )}

cos^{2} (a) - \frac{3}{5 sin ( a )}

元を分数に変換する:

cos^{2} (a) = \frac{cos ^{2} ( a ) 5 sin ( a )}{5 sin ( a )}

= \frac{cos ^{2} ( a ) \cdot 5 sin ( a )}{5 sin ( a )} - \frac{3}{5 sin ( a )}

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{cos ^{2} ( a ) \cdot 5 sin ( a ) - 3}{5 sin ( a )}

\frac{5 cos ^{2} ( a ) sin ( a ) - 3}{5 sin ( a )} = 0

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

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

三角関数の公式を使用して書き換える

- 3 + 5 cos^{2} (a) sin (a)

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)

= - 3 + 5 (1 - sin^{2} (a)) sin (a)

- 3 + (1 - sin^{2} (a)) \cdot 5 sin (a) = 0

置換で解く

- 3 + (1 - sin^{2} (a)) \cdot 5 sin (a) = 0

仮定:

sin (a) = u

- 3 + (1 - u^{2}) \cdot 5 u = 0

- 3 + (1 - u^{2}) \cdot 5 u = 0 : u \approx - 1.22119 \dots

- 3 + (1 - u^{2}) \cdot 5 u = 0

拡張

- 3 + (1 - u^{2}) \cdot 5 u : - 3 + 5 u - 5 u^{3}

- 3 + (1 - u^{2}) \cdot 5 u

= - 3 + 5 u (1 - u^{2})

拡張

5 u (1 - u^{2}) : 5 u - 5 u^{3}

5 u (1 - u^{2})

分配法則を適用する:

a (b - c) = ab - a c

a = 5 u, b = 1, c = u^{2}

= 5 u \cdot 1 - 5 u u^{2}

= 5 \cdot 1 \cdot u - 5 u^{2} u

簡素化

5 \cdot 1 \cdot u - 5 u^{2} u : 5 u - 5 u^{3}

5 \cdot 1 \cdot u - 5 u^{2} u

5 \cdot 1 \cdot u = 5 u

5 \cdot 1 \cdot u

数を乗じる:

5 \cdot 1 = 5

= 5 u

5 u^{2} u = 5 u^{3}

5 u^{2} u

指数の規則を適用する:

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

u^{2} u = u^{2 + 1}

= 5 u^{2 + 1}

数を足す:

2 + 1 = 3

= 5 u^{3}

= 5 u - 5 u^{3}

= 5 u - 5 u^{3}

= - 3 + 5 u - 5 u^{3}

- 3 + 5 u - 5 u^{3} = 0

標準的な形式で書く

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

- 5 u^{3} + 5 u - 3 = 0

ニュートン・ラプソン法を使用して

- 5 u^{3} + 5 u - 3 = 0

の解を1つ求める:

u \approx - 1.22119 \dots

- 5 u^{3} + 5 u - 3 = 0

ニュートン・ラプソン概算の定義

f (u) = - 5 u^{3} + 5 u - 3

発見する

f^{^{'}} (u) : - 15 u^{2} + 5

\frac{d}{d u} (- 5 u^{3} + 5 u - 3)

和/差の法則を適用:

(f \pm g)^{'} = f^{'} \pm g^{'}

= - \frac{d}{d u} (5 u^{3}) + \frac{d}{d u} (5 u) - \frac{d}{d u} (3)

\frac{d}{d u} (5 u^{3}) = 15 u^{2}

\frac{d}{d u} (5 u^{3})

定数を除去:

(a \cdot f)^{'} = a \cdot f^{'}

= 5 \frac{d}{d u} (u^{3})

乗の法則を適用:

\frac{d}{d x} (x^{a}) = a \cdot x^{a - 1}

= 5 \cdot 3 u^{3 - 1}

簡素化

= 15 u^{2}

\frac{d}{d u} (5 u) = 5

\frac{d}{d u} (5 u)

定数を除去:

(a \cdot f)^{'} = a \cdot f^{'}

= 5 \frac{d u}{d u}

共通の導関数を適用:

\frac{d u}{d u} = 1

= 5 \cdot 1

簡素化

= 5

\frac{d}{d u} (3) = 0

\frac{d}{d u} (3)

定数の導関数:

\frac{d}{d x} (a) = 0

= 0

= - 15 u^{2} + 5 - 0

簡素化

= - 15 u^{2} + 5

仮定:

u_{0} = - 1

Δ u_{n + 1} <

になるまで

u_{n + 1}

を計算する

0.000001

u_{1} = - 1.3 : Δ u_{1} = 0.3

f (u_{0}) = - 5 (- 1)^{3} + 5 (- 1) - 3 = - 3

f^{^{'}} (u_{0}) = - 15 (- 1)^{2} + 5 = - 10

u_{1} = - 1.3

Δ u_{1} = ∣ - 1.3 - (- 1) ∣ = 0.3

Δ u_{1} = 0.3

u_{2} = - 1.22702 \dots : Δ u_{2} = 0.07297 \dots

f (u_{1}) = - 5 (- 1.3)^{3} + 5 (- 1.3) - 3 = 1.485

f^{^{'}} (u_{1}) = - 15 (- 1.3)^{2} + 5 = - 20.35

u_{2} = - 1.22702 \dots

Δ u_{2} = ∣ - 1.22702 \dots - (- 1.3) ∣ = 0.07297 \dots

Δ u_{2} = 0.07297 \dots

u_{3} = - 1.22123 \dots : Δ u_{3} = 0.00579 \dots

f (u_{2}) = - 5 (- 1.22702 \dots)^{3} + 5 (- 1.22702 \dots) - 3 = 0.10189 \dots

f^{^{'}} (u_{2}) = - 15 (- 1.22702 \dots)^{2} + 5 = - 17.58392 \dots

u_{3} = - 1.22123 \dots

Δ u_{3} = ∣ - 1.22123 \dots - (- 1.22702 \dots) ∣ = 0.00579 \dots

Δ u_{3} = 0.00579 \dots

u_{4} = - 1.22119 \dots : Δ u_{4} = 0.00003 \dots

f (u_{3}) = - 5 (- 1.22123 \dots)^{3} + 5 (- 1.22123 \dots) - 3 = 0.00061 \dots

f^{^{'}} (u_{3}) = - 15 (- 1.22123 \dots)^{2} + 5 = - 17.37112 \dots

u_{4} = - 1.22119 \dots

Δ u_{4} = ∣ - 1.22119 \dots - (- 1.22123 \dots) ∣ = 0.00003 \dots

Δ u_{4} = 0.00003 \dots

u_{5} = - 1.22119 \dots : Δ u_{5} = 1.33081 E - 9

f (u_{4}) = - 5 (- 1.22119 \dots)^{3} + 5 (- 1.22119 \dots) - 3 = 2.31159 E - 8

f^{^{'}} (u_{4}) = - 15 (- 1.22119 \dots)^{2} + 5 = - 17.36982 \dots

u_{5} = - 1.22119 \dots

Δ u_{5} = ∣ - 1.22119 \dots - (- 1.22119 \dots) ∣ = 1.33081 E - 9

Δ u_{5} = 1.33081 E - 9

u \approx - 1.22119 \dots

長除法を適用する:

\frac{- 5 u ^{3} + 5 u - 3}{u + 1.22119 \dots} = - 5 u^{2} + 6.10598 \dots u - 2.45660 \dots

- 5 u^{2} + 6.10598 \dots u - 2.45660 \dots \approx 0

ニュートン・ラプソン法を使用して

- 5 u^{2} + 6.10598 \dots u - 2.45660 \dots = 0

の解を1つ求める:

以下の解はない:

u \in R

- 5 u^{2} + 6.10598 \dots u - 2.45660 \dots = 0

ニュートン・ラプソン概算の定義

f (u) = - 5 u^{2} + 6.10598 \dots u - 2.45660 \dots

発見する

f^{^{'}} (u) : - 10 u + 6.10598 \dots

\frac{d}{d u} (- 5 u^{2} + 6.10598 \dots u - 2.45660 \dots)

和/差の法則を適用:

(f \pm g)^{'} = f^{'} \pm g^{'}

= - \frac{d}{d u} (5 u^{2}) + \frac{d}{d u} (6.10598 \dots u) - \frac{d}{d u} (2.45660 \dots)

\frac{d}{d u} (5 u^{2}) = 10 u

\frac{d}{d u} (5 u^{2})

定数を除去:

(a \cdot f)^{'} = a \cdot f^{'}

= 5 \frac{d}{d u} (u^{2})

乗の法則を適用:

\frac{d}{d x} (x^{a}) = a \cdot x^{a - 1}

= 5 \cdot 2 u^{2 - 1}

簡素化

= 10 u

\frac{d}{d u} (6.10598 \dots u) = 6.10598 \dots

\frac{d}{d u} (6.10598 \dots u)

定数を除去:

(a \cdot f)^{'} = a \cdot f^{'}

= 6.10598 \dots \frac{d u}{d u}

共通の導関数を適用:

\frac{d u}{d u} = 1

= 6.10598 \dots \cdot 1

簡素化

= 6.10598 \dots

\frac{d}{d u} (2.45660 \dots) = 0

\frac{d}{d u} (2.45660 \dots)

定数の導関数:

\frac{d}{d x} (a) = 0

= 0

= - 10 u + 6.10598 \dots - 0

簡素化

= - 10 u + 6.10598 \dots

仮定:

u_{0} = 0

Δ u_{n + 1} <

になるまで

u_{n + 1}

を計算する

0.000001

u_{1} = 0.40232 \dots : Δ u_{1} = 0.40232 \dots

f (u_{0}) = - 5 \cdot 0^{2} + 6.10598 \dots \cdot 0 - 2.45660 \dots = - 2.45660 \dots

f^{^{'}} (u_{0}) = - 10 \cdot 0 + 6.10598 \dots = 6.10598 \dots

u_{1} = 0.40232 \dots

Δ u_{1} = ∣ 0.40232 \dots - 0 ∣ = 0.40232 \dots

Δ u_{1} = 0.40232 \dots

u_{2} = 0.79092 \dots : Δ u_{2} = 0.38859 \dots

f (u_{1}) = - 5 \cdot 0.40232 \dots^{2} + 6.10598 \dots \cdot 0.40232 \dots - 2.45660 \dots = - 0.80933 \dots

f^{^{'}} (u_{1}) = - 10 \cdot 0.40232 \dots + 6.10598 \dots = 2.08270 \dots

u_{2} = 0.79092 \dots

Δ u_{2} = ∣ 0.79092 \dots - 0.40232 \dots ∣ = 0.38859 \dots

Δ u_{2} = 0.38859 \dots

u_{3} = 0.37222 \dots : Δ u_{3} = 0.41870 \dots

f (u_{2}) = - 5 \cdot 0.79092 \dots^{2} + 6.10598 \dots \cdot 0.79092 \dots - 2.45660 \dots = - 0.75504 \dots

f^{^{'}} (u_{2}) = - 10 \cdot 0.79092 \dots + 6.10598 \dots = - 1.80328 \dots

u_{3} = 0.37222 \dots

Δ u_{3} = ∣ 0.37222 \dots - 0.79092 \dots ∣ = 0.41870 \dots

Δ u_{3} = 0.41870 \dots

u_{4} = 0.73994 \dots : Δ u_{4} = 0.36772 \dots

f (u_{3}) = - 5 \cdot 0.37222 \dots^{2} + 6.10598 \dots \cdot 0.37222 \dots - 2.45660 \dots = - 0.87657 \dots

f^{^{'}} (u_{3}) = - 10 \cdot 0.37222 \dots + 6.10598 \dots = 2.38377 \dots

u_{4} = 0.73994 \dots

Δ u_{4} = ∣ 0.73994 \dots - 0.37222 \dots ∣ = 0.36772 \dots

Δ u_{4} = 0.36772 \dots

u_{5} = 0.21724 \dots : Δ u_{5} = 0.52270 \dots

f (u_{4}) = - 5 \cdot 0.73994 \dots^{2} + 6.10598 \dots \cdot 0.73994 \dots - 2.45660 \dots = - 0.67611 \dots

f^{^{'}} (u_{4}) = - 10 \cdot 0.73994 \dots + 6.10598 \dots = - 1.29348 \dots

u_{5} = 0.21724 \dots

Δ u_{5} = ∣ 0.21724 \dots - 0.73994 \dots ∣ = 0.52270 \dots

Δ u_{5} = 0.52270 \dots

u_{6} = 0.56453 \dots : Δ u_{6} = 0.34729 \dots

f (u_{5}) = - 5 \cdot 0.21724 \dots^{2} + 6.10598 \dots \cdot 0.21724 \dots - 2.45660 \dots = - 1.36610 \dots

f^{^{'}} (u_{5}) = - 10 \cdot 0.21724 \dots + 6.10598 \dots = 3.93356 \dots

u_{6} = 0.56453 \dots

Δ u_{6} = ∣ 0.56453 \dots - 0.21724 \dots ∣ = 0.34729 \dots

Δ u_{6} = 0.34729 \dots

u_{7} = 1.87375 \dots : Δ u_{7} = 1.30922 \dots

f (u_{6}) = - 5 \cdot 0.56453 \dots^{2} + 6.10598 \dots \cdot 0.56453 \dots - 2.45660 \dots = - 0.60306 \dots

f^{^{'}} (u_{6}) = - 10 \cdot 0.56453 \dots + 6.10598 \dots = 0.46062 \dots

u_{7} = 1.87375 \dots

Δ u_{7} = ∣ 1.87375 \dots - 0.56453 \dots ∣ = 1.30922 \dots

Δ u_{7} = 1.30922 \dots

u_{8} = 1.19527 \dots : Δ u_{8} = 0.67848 \dots

f (u_{7}) = - 5 \cdot 1.87375 \dots^{2} + 6.10598 \dots \cdot 1.87375 \dots - 2.45660 \dots = - 8.57033 \dots

f^{^{'}} (u_{7}) = - 10 \cdot 1.87375 \dots + 6.10598 \dots = - 12.63161 \dots

u_{8} = 1.19527 \dots

Δ u_{8} = ∣ 1.19527 \dots - 1.87375 \dots ∣ = 0.67848 \dots

Δ u_{8} = 0.67848 \dots

u_{9} = 0.80160 \dots : Δ u_{9} = 0.39366 \dots

f (u_{8}) = - 5 \cdot 1.19527 \dots^{2} + 6.10598 \dots \cdot 1.19527 \dots - 2.45660 \dots = - 2.30169 \dots

f^{^{'}} (u_{8}) = - 10 \cdot 1.19527 \dots + 6.10598 \dots = - 5.84678 \dots

u_{9} = 0.80160 \dots

Δ u_{9} = ∣ 0.80160 \dots - 1.19527 \dots ∣ = 0.39366 \dots

Δ u_{9} = 0.39366 \dots

u_{10} = 0.39593 \dots : Δ u_{10} = 0.40567 \dots

f (u_{9}) = - 5 \cdot 0.80160 \dots^{2} + 6.10598 \dots \cdot 0.80160 \dots - 2.45660 \dots = - 0.77487 \dots

f^{^{'}} (u_{9}) = - 10 \cdot 0.80160 \dots + 6.10598 \dots = - 1.91008 \dots

u_{10} = 0.39593 \dots

Δ u_{10} = ∣ 0.39593 \dots - 0.80160 \dots ∣ = 0.40567 \dots

Δ u_{10} = 0.40567 \dots

解を見つけられない

解は

u \approx - 1.22119 \dots

代用を戻す

u = sin (a)

sin (a) \approx - 1.22119 \dots

sin (a) \approx - 1.22119 \dots

sin (a) = - 1.22119 \dots :

解なし

sin (a) = - 1.22119 \dots

- 1 \leq sin (x) \leq 1

解なし

すべての解を組み合わせる

以下の解はない : a \in R

グラフ

人気の例

3cos(x)=2sec(x)-5

3 cos (x) = 2 sec (x) - 5

sin(a/2)=(1/2)sin(a)

sin (\frac{a}{2}) = (\frac{1}{2}) sin (a)

cos(x/2)=cos(x)+1

cos (\frac{x}{2}) = cos (x) + 1

d=(sin^4(x)-cos^2(x)+5)/(4*cos^2(x))

d = \frac{sin ^{4} ( x ) - cos ^{2} ( x ) + 5}{4 \cdot cos ^{2} ( x )}

2+cos^2(x)=5sin(x)

2 + cos^{2} (x) = 5 sin (x)