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Popolare Trigonometria >

cos^4(x)=cos^{23}(x)

Soluzione

cos^{4} (x) = cos^{23} (x)

Soluzione

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

Gradi

x = 9 0^{\circ} + 36 0^{\circ} n, x = 27 0^{\circ} + 36 0^{\circ} n, x = 0^{\circ} + 36 0^{\circ} n

Fasi della soluzione

cos^{4} (x) = cos^{23} (x)

Risolvi per sostituzione

cos^{4} (x) = cos^{23} (x)

Sia:

cos (x) = u

u^{4} = u^{23}

u^{4} = u^{23} : u = 0, u = 1

u^{4} = u^{23}

Scambia i lati

u^{23} = u^{4}

Spostare

u^{4}

a sinistra dell'equazione

u^{23} = u^{4}

Sottrarre

u^{4}

da entrambi i lati

u^{23} - u^{4} = u^{4} - u^{4}

Semplificare

u^{23} - u^{4} = 0

u^{23} - u^{4} = 0

Fattorizza

u^{23} - u^{4} : u^{4} (u - 1) (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1)

u^{23} - u^{4}

Fattorizzare dal termine comune

u^{4} : u^{4} (u^{19} - 1)

u^{23} - u^{4}

Applica la regola degli esponenti:

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

u^{23} = u^{19} u^{4}

= u^{19} u^{4} - u^{4}

Fattorizzare dal termine comune

u^{4}

= u^{4} (u^{19} - 1)

= u^{4} (u^{19} - 1)

Fattorizza

u^{19} - 1 : (u - 1) (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1)

u^{19} - 1

Riscrivi

1

come

1^{19}

= u^{19} - 1^{19}

Applicare la regola di fattorizzazione:

x^{n} - y^{n} = (x - y) (x^{n - 1} + x^{n - 2} y + \dots + x y^{n - 2} y^{n - 1})

u^{19} - 1^{19} = (u - 1) (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1)

= (u - 1) (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1)

= u^{4} (u - 1) (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1)

u^{4} (u - 1) (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1) = 0

Usando il Principio del Fattore Zero:

ab = 0

allora

a = 0

b = 0

u = 0 or u - 1 = 0 or u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1 = 0

Risolvi

u - 1 = 0 : u = 1

u - 1 = 0

Spostare

1

a destra dell'equazione

u - 1 = 0

Aggiungi

1

ad entrambi i lati

u - 1 + 1 = 0 + 1

Semplificare

u = 1

u = 1

Risolvi

u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1 = 0 :

Nessuna soluzione per

u \in R

u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1 = 0

Trova una soluzione per

u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1 = 0

utilizzando Newton-Raphson:

Nessuna soluzione per

u \in R

u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1 = 0

Definizione di approssimazione di Newton-Raphson

f (u) = u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1

Trova

f^{^{'}} (u) : 18 u^{17} + 17 u^{16} + 16 u^{15} + 15 u^{14} + 14 u^{13} + 13 u^{12} + 12 u^{11} + 11 u^{10} + 10 u^{9} + 9 u^{8} + 8 u^{7} + 7 u^{6} + 6 u^{5} + 5 u^{4} + 4 u^{3} + 3 u^{2} + 2 u + 1

\frac{d}{d u} (u^{18} + u^{17} + u^{16} + u^{15} + u^{14} + u^{13} + u^{12} + u^{11} + u^{10} + u^{9} + u^{8} + u^{7} + u^{6} + u^{5} + u^{4} + u^{3} + u^{2} + u + 1)

Applica la regola della somma/differenza:

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

= \frac{d}{d u} (u^{18}) + \frac{d}{d u} (u^{17}) + \frac{d}{d u} (u^{16}) + \frac{d}{d u} (u^{15}) + \frac{d}{d u} (u^{14}) + \frac{d}{d u} (u^{13}) + \frac{d}{d u} (u^{12}) + \frac{d}{d u} (u^{11}) + \frac{d}{d u} (u^{10}) + \frac{d}{d u} (u^{9}) + \frac{d}{d u} (u^{8}) + \frac{d}{d u} (u^{7}) + \frac{d}{d u} (u^{6}) + \frac{d}{d u} (u^{5}) + \frac{d}{d u} (u^{4}) + \frac{d}{d u} (u^{3}) + \frac{d}{d u} (u^{2}) + \frac{d u}{d u} + \frac{d}{d u} (1)

\frac{d}{d u} (u^{18}) = 18 u^{17}

\frac{d}{d u} (u^{18})

Applica la regola della potenza:

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

= 18 u^{18 - 1}

Semplificare

= 18 u^{17}

\frac{d}{d u} (u^{17}) = 17 u^{16}

\frac{d}{d u} (u^{17})

Applica la regola della potenza:

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

= 17 u^{17 - 1}

Semplificare

= 17 u^{16}

\frac{d}{d u} (u^{16}) = 16 u^{15}

\frac{d}{d u} (u^{16})

Applica la regola della potenza:

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

= 16 u^{16 - 1}

Semplificare

= 16 u^{15}

\frac{d}{d u} (u^{15}) = 15 u^{14}

\frac{d}{d u} (u^{15})

Applica la regola della potenza:

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

= 15 u^{15 - 1}

Semplificare

= 15 u^{14}

\frac{d}{d u} (u^{14}) = 14 u^{13}

\frac{d}{d u} (u^{14})

Applica la regola della potenza:

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

= 14 u^{14 - 1}

Semplificare

= 14 u^{13}

\frac{d}{d u} (u^{13}) = 13 u^{12}

\frac{d}{d u} (u^{13})

Applica la regola della potenza:

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

= 13 u^{13 - 1}

Semplificare

= 13 u^{12}

\frac{d}{d u} (u^{12}) = 12 u^{11}

\frac{d}{d u} (u^{12})

Applica la regola della potenza:

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

= 12 u^{12 - 1}

Semplificare

= 12 u^{11}

\frac{d}{d u} (u^{11}) = 11 u^{10}

\frac{d}{d u} (u^{11})

Applica la regola della potenza:

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

= 11 u^{11 - 1}

Semplificare

= 11 u^{10}

\frac{d}{d u} (u^{10}) = 10 u^{9}

\frac{d}{d u} (u^{10})

Applica la regola della potenza:

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

= 10 u^{10 - 1}

Semplificare

= 10 u^{9}

\frac{d}{d u} (u^{9}) = 9 u^{8}

\frac{d}{d u} (u^{9})

Applica la regola della potenza:

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

= 9 u^{9 - 1}

Semplificare

= 9 u^{8}

\frac{d}{d u} (u^{8}) = 8 u^{7}

\frac{d}{d u} (u^{8})

Applica la regola della potenza:

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

= 8 u^{8 - 1}

Semplificare

= 8 u^{7}

\frac{d}{d u} (u^{7}) = 7 u^{6}

\frac{d}{d u} (u^{7})

Applica la regola della potenza:

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

= 7 u^{7 - 1}

Semplificare

= 7 u^{6}

\frac{d}{d u} (u^{6}) = 6 u^{5}

\frac{d}{d u} (u^{6})

Applica la regola della potenza:

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

= 6 u^{6 - 1}

Semplificare

= 6 u^{5}

\frac{d}{d u} (u^{5}) = 5 u^{4}

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

Applica la regola della potenza:

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

= 5 u^{5 - 1}

Semplificare

= 5 u^{4}

\frac{d}{d u} (u^{4}) = 4 u^{3}

\frac{d}{d u} (u^{4})

Applica la regola della potenza:

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

= 4 u^{4 - 1}

Semplificare

= 4 u^{3}

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

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

Applica la regola della potenza:

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

= 3 u^{3 - 1}

Semplificare

= 3 u^{2}

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

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

Applica la regola della potenza:

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

= 2 u^{2 - 1}

Semplificare

= 2 u

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

\frac{d u}{d u}

Applica la derivata comune:

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

= 1

\frac{d}{d u} (1) = 0

\frac{d}{d u} (1)

Derivata di una costante:

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

= 0

= 18 u^{17} + 17 u^{16} + 16 u^{15} + 15 u^{14} + 14 u^{13} + 13 u^{12} + 12 u^{11} + 11 u^{10} + 10 u^{9} + 9 u^{8} + 8 u^{7} + 7 u^{6} + 6 u^{5} + 5 u^{4} + 4 u^{3} + 3 u^{2} + 2 u + 1 + 0

Semplificare

= 18 u^{17} + 17 u^{16} + 16 u^{15} + 15 u^{14} + 14 u^{13} + 13 u^{12} + 12 u^{11} + 11 u^{10} + 10 u^{9} + 9 u^{8} + 8 u^{7} + 7 u^{6} + 6 u^{5} + 5 u^{4} + 4 u^{3} + 3 u^{2} + 2 u + 1

Sia

u_{0} = - 1

Calcola

u_{n + 1}

fino a

De lt a u_{n + 1} < 0.000001

u_{1} = - 0.88888 \dots : Δ u_{1} = 0.11111 \dots

f (u_{0}) = (- 1)^{18} + (- 1)^{17} + (- 1)^{16} + (- 1)^{15} + (- 1)^{14} + (- 1)^{13} + (- 1)^{12} + (- 1)^{11} + (- 1)^{10} + (- 1)^{9} + (- 1)^{8} + (- 1)^{7} + (- 1)^{6} + (- 1)^{5} + (- 1)^{4} + (- 1)^{3} + (- 1)^{2} + (- 1) + 1 = 1

f^{^{'}} (u_{0}) = 18 (- 1)^{17} + 17 (- 1)^{16} + 16 (- 1)^{15} + 15 (- 1)^{14} + 14 (- 1)^{13} + 13 (- 1)^{12} + 12 (- 1)^{11} + 11 (- 1)^{10} + 10 (- 1)^{9} + 9 (- 1)^{8} + 8 (- 1)^{7} + 7 (- 1)^{6} + 6 (- 1)^{5} + 5 (- 1)^{4} + 4 (- 1)^{3} + 3 (- 1)^{2} + 2 (- 1) + 1 = - 9

u_{1} = - 0.88888 \dots

Δ u_{1} = ∣ - 0.88888 \dots - (- 1) ∣ = 0.11111 \dots

Δ u_{1} = 0.11111 \dots

u_{2} = - 0.23578 \dots : Δ u_{2} = 0.65310 \dots

f (u_{1}) = (- 0.88888 \dots)^{18} + (- 0.88888 \dots)^{17} + (- 0.88888 \dots)^{16} + (- 0.88888 \dots)^{15} + (- 0.88888 \dots)^{14} + (- 0.88888 \dots)^{13} + (- 0.88888 \dots)^{12} + (- 0.88888 \dots)^{11} + (- 0.88888 \dots)^{10} + (- 0.88888 \dots)^{9} + (- 0.88888 \dots)^{8} + (- 0.88888 \dots)^{7} + (- 0.88888 \dots)^{6} + (- 0.88888 \dots)^{5} + (- 0.88888 \dots)^{4} + (- 0.88888 \dots)^{3} + (- 0.88888 \dots)^{2} + (- 0.88888 \dots) + 1 = 0.58589 \dots

f^{^{'}} (u_{1}) = 18 (- 0.88888 \dots)^{17} + 17 (- 0.88888 \dots)^{16} + 16 (- 0.88888 \dots)^{15} + 15 (- 0.88888 \dots)^{14} + 14 (- 0.88888 \dots)^{13} + 13 (- 0.88888 \dots)^{12} + 12 (- 0.88888 \dots)^{11} + 11 (- 0.88888 \dots)^{10} + 10 (- 0.88888 \dots)^{9} + 9 (- 0.88888 \dots)^{8} + 8 (- 0.88888 \dots)^{7} + 7 (- 0.88888 \dots)^{6} + 6 (- 0.88888 \dots)^{5} + 5 (- 0.88888 \dots)^{4} + 4 (- 0.88888 \dots)^{3} + 3 (- 0.88888 \dots)^{2} + 2 (- 0.88888 \dots) + 1 = - 0.89708 \dots

u_{2} = - 0.23578 \dots

Δ u_{2} = ∣ - 0.23578 \dots - (- 0.88888 \dots) ∣ = 0.65310 \dots

Δ u_{2} = 0.65310 \dots

u_{3} = - 1.47156 \dots : Δ u_{3} = 1.23578 \dots

f (u_{2}) = (- 0.23578 \dots)^{18} + (- 0.23578 \dots)^{17} + (- 0.23578 \dots)^{16} + (- 0.23578 \dots)^{15} + (- 0.23578 \dots)^{14} + (- 0.23578 \dots)^{13} + (- 0.23578 \dots)^{12} + (- 0.23578 \dots)^{11} + (- 0.23578 \dots)^{10} + (- 0.23578 \dots)^{9} + (- 0.23578 \dots)^{8} + (- 0.23578 \dots)^{7} + (- 0.23578 \dots)^{6} + (- 0.23578 \dots)^{5} + (- 0.23578 \dots)^{4} + (- 0.23578 \dots)^{3} + (- 0.23578 \dots)^{2} + (- 0.23578 \dots) + 1 = 0.80920 \dots

f^{^{'}} (u_{2}) = 18 (- 0.23578 \dots)^{17} + 17 (- 0.23578 \dots)^{16} + 16 (- 0.23578 \dots)^{15} + 15 (- 0.23578 \dots)^{14} + 14 (- 0.23578 \dots)^{13} + 13 (- 0.23578 \dots)^{12} + 12 (- 0.23578 \dots)^{11} + 11 (- 0.23578 \dots)^{10} + 10 (- 0.23578 \dots)^{9} + 9 (- 0.23578 \dots)^{8} + 8 (- 0.23578 \dots)^{7} + 7 (- 0.23578 \dots)^{6} + 6 (- 0.23578 \dots)^{5} + 5 (- 0.23578 \dots)^{4} + 4 (- 0.23578 \dots)^{3} + 3 (- 0.23578 \dots)^{2} + 2 (- 0.23578 \dots) + 1 = 0.65481 \dots

u_{3} = - 1.47156 \dots

Δ u_{3} = ∣ - 1.47156 \dots - (- 0.23578 \dots) ∣ = 1.23578 \dots

Δ u_{3} = 1.23578 \dots

u_{4} = - 1.39155 \dots : Δ u_{4} = 0.08000 \dots

f (u_{3}) = (- 1.47156 \dots)^{18} + (- 1.47156 \dots)^{17} + (- 1.47156 \dots)^{16} + (- 1.47156 \dots)^{15} + (- 1.47156 \dots)^{14} + (- 1.47156 \dots)^{13} + (- 1.47156 \dots)^{12} + (- 1.47156 \dots)^{11} + (- 1.47156 \dots)^{10} + (- 1.47156 \dots)^{9} + (- 1.47156 \dots)^{8} + (- 1.47156 \dots)^{7} + (- 1.47156 \dots)^{6} + (- 1.47156 \dots)^{5} + (- 1.47156 \dots)^{4} + (- 1.47156 \dots)^{3} + (- 1.47156 \dots)^{2} + (- 1.47156 \dots) + 1 = 623.90302 \dots

f^{^{'}} (u_{3}) = 18 (- 1.47156 \dots)^{17} + 17 (- 1.47156 \dots)^{16} + 16 (- 1.47156 \dots)^{15} + 15 (- 1.47156 \dots)^{14} + 14 (- 1.47156 \dots)^{13} + 13 (- 1.47156 \dots)^{12} + 12 (- 1.47156 \dots)^{11} + 11 (- 1.47156 \dots)^{10} + 10 (- 1.47156 \dots)^{9} + 9 (- 1.47156 \dots)^{8} + 8 (- 1.47156 \dots)^{7} + 7 (- 1.47156 \dots)^{6} + 6 (- 1.47156 \dots)^{5} + 5 (- 1.47156 \dots)^{4} + 4 (- 1.47156 \dots)^{3} + 3 (- 1.47156 \dots)^{2} + 2 (- 1.47156 \dots) + 1 = - 7797.82245 \dots

u_{4} = - 1.39155 \dots

Δ u_{4} = ∣ - 1.39155 \dots - (- 1.47156 \dots) ∣ = 0.08000 \dots

Δ u_{4} = 0.08000 \dots

u_{5} = - 1.31585 \dots : Δ u_{5} = 0.07569 \dots

f (u_{4}) = (- 1.39155 \dots)^{18} + (- 1.39155 \dots)^{17} + (- 1.39155 \dots)^{16} + (- 1.39155 \dots)^{15} + (- 1.39155 \dots)^{14} + (- 1.39155 \dots)^{13} + (- 1.39155 \dots)^{12} + (- 1.39155 \dots)^{11} + (- 1.39155 \dots)^{10} + (- 1.39155 \dots)^{9} + (- 1.39155 \dots)^{8} + (- 1.39155 \dots)^{7} + (- 1.39155 \dots)^{6} + (- 1.39155 \dots)^{5} + (- 1.39155 \dots)^{4} + (- 1.39155 \dots)^{3} + (- 1.39155 \dots)^{2} + (- 1.39155 \dots) + 1 = 223.17190 \dots

f^{^{'}} (u_{4}) = 18 (- 1.39155 \dots)^{17} + 17 (- 1.39155 \dots)^{16} + 16 (- 1.39155 \dots)^{15} + 15 (- 1.39155 \dots)^{14} + 14 (- 1.39155 \dots)^{13} + 13 (- 1.39155 \dots)^{12} + 12 (- 1.39155 \dots)^{11} + 11 (- 1.39155 \dots)^{10} + 10 (- 1.39155 \dots)^{9} + 9 (- 1.39155 \dots)^{8} + 8 (- 1.39155 \dots)^{7} + 7 (- 1.39155 \dots)^{6} + 6 (- 1.39155 \dots)^{5} + 5 (- 1.39155 \dots)^{4} + 4 (- 1.39155 \dots)^{3} + 3 (- 1.39155 \dots)^{2} + 2 (- 1.39155 \dots) + 1 = - 2948.11712 \dots

u_{5} = - 1.31585 \dots

Δ u_{5} = ∣ - 1.31585 \dots - (- 1.39155 \dots) ∣ = 0.07569 \dots

Δ u_{5} = 0.07569 \dots

u_{6} = - 1.24406 \dots : Δ u_{6} = 0.07179 \dots

f (u_{5}) = (- 1.31585 \dots)^{18} + (- 1.31585 \dots)^{17} + (- 1.31585 \dots)^{16} + (- 1.31585 \dots)^{15} + (- 1.31585 \dots)^{14} + (- 1.31585 \dots)^{13} + (- 1.31585 \dots)^{12} + (- 1.31585 \dots)^{11} + (- 1.31585 \dots)^{10} + (- 1.31585 \dots)^{9} + (- 1.31585 \dots)^{8} + (- 1.31585 \dots)^{7} + (- 1.31585 \dots)^{6} + (- 1.31585 \dots)^{5} + (- 1.31585 \dots)^{4} + (- 1.31585 \dots)^{3} + (- 1.31585 \dots)^{2} + (- 1.31585 \dots) + 1 = 79.90865 \dots

f^{^{'}} (u_{5}) = 18 (- 1.31585 \dots)^{17} + 17 (- 1.31585 \dots)^{16} + 16 (- 1.31585 \dots)^{15} + 15 (- 1.31585 \dots)^{14} + 14 (- 1.31585 \dots)^{13} + 13 (- 1.31585 \dots)^{12} + 12 (- 1.31585 \dots)^{11} + 11 (- 1.31585 \dots)^{10} + 10 (- 1.31585 \dots)^{9} + 9 (- 1.31585 \dots)^{8} + 8 (- 1.31585 \dots)^{7} + 7 (- 1.31585 \dots)^{6} + 6 (- 1.31585 \dots)^{5} + 5 (- 1.31585 \dots)^{4} + 4 (- 1.31585 \dots)^{3} + 3 (- 1.31585 \dots)^{2} + 2 (- 1.31585 \dots) + 1 = - 1113.08361 \dots

u_{6} = - 1.24406 \dots

Δ u_{6} = ∣ - 1.24406 \dots - (- 1.31585 \dots) ∣ = 0.07179 \dots

Δ u_{6} = 0.07179 \dots

u_{7} = - 1.17552 \dots : Δ u_{7} = 0.06854 \dots

f (u_{6}) = (- 1.24406 \dots)^{18} + (- 1.24406 \dots)^{17} + (- 1.24406 \dots)^{16} + (- 1.24406 \dots)^{15} + (- 1.24406 \dots)^{14} + (- 1.24406 \dots)^{13} + (- 1.24406 \dots)^{12} + (- 1.24406 \dots)^{11} + (- 1.24406 \dots)^{10} + (- 1.24406 \dots)^{9} + (- 1.24406 \dots)^{8} + (- 1.24406 \dots)^{7} + (- 1.24406 \dots)^{6} + (- 1.24406 \dots)^{5} + (- 1.24406 \dots)^{4} + (- 1.24406 \dots)^{3} + (- 1.24406 \dots)^{2} + (- 1.24406 \dots) + 1 = 28.69312 \dots

f^{^{'}} (u_{6}) = 18 (- 1.24406 \dots)^{17} + 17 (- 1.24406 \dots)^{16} + 16 (- 1.24406 \dots)^{15} + 15 (- 1.24406 \dots)^{14} + 14 (- 1.24406 \dots)^{13} + 13 (- 1.24406 \dots)^{12} + 12 (- 1.24406 \dots)^{11} + 11 (- 1.24406 \dots)^{10} + 10 (- 1.24406 \dots)^{9} + 9 (- 1.24406 \dots)^{8} + 8 (- 1.24406 \dots)^{7} + 7 (- 1.24406 \dots)^{6} + 6 (- 1.24406 \dots)^{5} + 5 (- 1.24406 \dots)^{4} + 4 (- 1.24406 \dots)^{3} + 3 (- 1.24406 \dots)^{2} + 2 (- 1.24406 \dots) + 1 = - 418.62427 \dots

u_{7} = - 1.17552 \dots

Δ u_{7} = ∣ - 1.17552 \dots - (- 1.24406 \dots) ∣ = 0.06854 \dots

Δ u_{7} = 0.06854 \dots

u_{8} = - 1.10880 \dots : Δ u_{8} = 0.06671 \dots

f (u_{7}) = (- 1.17552 \dots)^{18} + (- 1.17552 \dots)^{17} + (- 1.17552 \dots)^{16} + (- 1.17552 \dots)^{15} + (- 1.17552 \dots)^{14} + (- 1.17552 \dots)^{13} + (- 1.17552 \dots)^{12} + (- 1.17552 \dots)^{11} + (- 1.17552 \dots)^{10} + (- 1.17552 \dots)^{9} + (- 1.17552 \dots)^{8} + (- 1.17552 \dots)^{7} + (- 1.17552 \dots)^{6} + (- 1.17552 \dots)^{5} + (- 1.17552 \dots)^{4} + (- 1.17552 \dots)^{3} + (- 1.17552 \dots)^{2} + (- 1.17552 \dots) + 1 = 10.38689 \dots

f^{^{'}} (u_{7}) = 18 (- 1.17552 \dots)^{17} + 17 (- 1.17552 \dots)^{16} + 16 (- 1.17552 \dots)^{15} + 15 (- 1.17552 \dots)^{14} + 14 (- 1.17552 \dots)^{13} + 13 (- 1.17552 \dots)^{12} + 12 (- 1.17552 \dots)^{11} + 11 (- 1.17552 \dots)^{10} + 10 (- 1.17552 \dots)^{9} + 9 (- 1.17552 \dots)^{8} + 8 (- 1.17552 \dots)^{7} + 7 (- 1.17552 \dots)^{6} + 6 (- 1.17552 \dots)^{5} + 5 (- 1.17552 \dots)^{4} + 4 (- 1.17552 \dots)^{3} + 3 (- 1.17552 \dots)^{2} + 2 (- 1.17552 \dots) + 1 = - 155.67966 \dots

u_{8} = - 1.10880 \dots

Δ u_{8} = ∣ - 1.10880 \dots - (- 1.17552 \dots) ∣ = 0.06671 \dots

Δ u_{8} = 0.06671 \dots

u_{9} = - 1.04007 \dots : Δ u_{9} = 0.06872 \dots

f (u_{8}) = (- 1.10880 \dots)^{18} + (- 1.10880 \dots)^{17} + (- 1.10880 \dots)^{16} + (- 1.10880 \dots)^{15} + (- 1.10880 \dots)^{14} + (- 1.10880 \dots)^{13} + (- 1.10880 \dots)^{12} + (- 1.10880 \dots)^{11} + (- 1.10880 \dots)^{10} + (- 1.10880 \dots)^{9} + (- 1.10880 \dots)^{8} + (- 1.10880 \dots)^{7} + (- 1.10880 \dots)^{6} + (- 1.10880 \dots)^{5} + (- 1.10880 \dots)^{4} + (- 1.10880 \dots)^{3} + (- 1.10880 \dots)^{2} + (- 1.10880 \dots) + 1 = 3.84863 \dots

f^{^{'}} (u_{8}) = 18 (- 1.10880 \dots)^{17} + 17 (- 1.10880 \dots)^{16} + 16 (- 1.10880 \dots)^{15} + 15 (- 1.10880 \dots)^{14} + 14 (- 1.10880 \dots)^{13} + 13 (- 1.10880 \dots)^{12} + 12 (- 1.10880 \dots)^{11} + 11 (- 1.10880 \dots)^{10} + 10 (- 1.10880 \dots)^{9} + 9 (- 1.10880 \dots)^{8} + 8 (- 1.10880 \dots)^{7} + 7 (- 1.10880 \dots)^{6} + 6 (- 1.10880 \dots)^{5} + 5 (- 1.10880 \dots)^{4} + 4 (- 1.10880 \dots)^{3} + 3 (- 1.10880 \dots)^{2} + 2 (- 1.10880 \dots) + 1 = - 55.99781 \dots

u_{9} = - 1.04007 \dots

Δ u_{9} = ∣ - 1.04007 \dots - (- 1.10880 \dots) ∣ = 0.06872 \dots

Δ u_{9} = 0.06872 \dots

u_{10} = - 0.95606 \dots : Δ u_{10} = 0.08401 \dots

f (u_{9}) = (- 1.04007 \dots)^{18} + (- 1.04007 \dots)^{17} + (- 1.04007 \dots)^{16} + (- 1.04007 \dots)^{15} + (- 1.04007 \dots)^{14} + (- 1.04007 \dots)^{13} + (- 1.04007 \dots)^{12} + (- 1.04007 \dots)^{11} + (- 1.04007 \dots)^{10} + (- 1.04007 \dots)^{9} + (- 1.04007 \dots)^{8} + (- 1.04007 \dots)^{7} + (- 1.04007 \dots)^{6} + (- 1.04007 \dots)^{5} + (- 1.04007 \dots)^{4} + (- 1.04007 \dots)^{3} + (- 1.04007 \dots)^{2} + (- 1.04007 \dots) + 1 = 1.52432 \dots

f^{^{'}} (u_{9}) = 18 (- 1.04007 \dots)^{17} + 17 (- 1.04007 \dots)^{16} + 16 (- 1.04007 \dots)^{15} + 15 (- 1.04007 \dots)^{14} + 14 (- 1.04007 \dots)^{13} + 13 (- 1.04007 \dots)^{12} + 12 (- 1.04007 \dots)^{11} + 11 (- 1.04007 \dots)^{10} + 10 (- 1.04007 \dots)^{9} + 9 (- 1.04007 \dots)^{8} + 8 (- 1.04007 \dots)^{7} + 7 (- 1.04007 \dots)^{6} + 6 (- 1.04007 \dots)^{5} + 5 (- 1.04007 \dots)^{4} + 4 (- 1.04007 \dots)^{3} + 3 (- 1.04007 \dots)^{2} + 2 (- 1.04007 \dots) + 1 = - 18.14456 \dots

u_{10} = - 0.95606 \dots

Δ u_{10} = ∣ - 0.95606 \dots - (- 1.04007 \dots) ∣ = 0.08401 \dots

Δ u_{10} = 0.08401 \dots

Non è possibile trovare soluzione

La soluzione è

Nessuna soluzione per u \in R

Le soluzioni sono

u = 0, u = 1

Sostituire indietro

u = cos (x)

cos (x) = 0, cos (x) = 1

cos (x) = 0, cos (x) = 1

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

cos (x) = 0

Soluzioni generali per

cos (x) = 0

cos (x)

periodicità tabella con

2 πn

cicli:

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} cos (x) 1 \frac{3}{2} \frac{2}{2} \frac{1}{2} 0 - \frac{1}{2} - \frac{2}{2} - \frac{3}{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} cos (x) - 1 - \frac{3}{2} - \frac{2}{2} - \frac{1}{2} 0 \frac{1}{2} \frac{2}{2} \frac{3}{2}

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

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

cos (x) = 1 : x = 2 πn

cos (x) = 1

Soluzioni generali per

cos (x) = 1

cos (x)

periodicità tabella con

2 πn

cicli:

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} cos (x) 1 \frac{3}{2} \frac{2}{2} \frac{1}{2} 0 - \frac{1}{2} - \frac{2}{2} - \frac{3}{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} cos (x) - 1 - \frac{3}{2} - \frac{2}{2} - \frac{1}{2} 0 \frac{1}{2} \frac{2}{2} \frac{3}{2}

x = 0 + 2 πn

x = 0 + 2 πn

Risolvi

x = 0 + 2 πn : x = 2 πn

x = 0 + 2 πn

0 + 2 πn = 2 πn

x = 2 πn

x = 2 πn

Combinare tutte le soluzioni

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

Grafico

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