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Popular Trigonometry >

sin^3(x)+sin(x)-4=0

  • Pre Algebra
  • Algebra
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Solution

sin3(x)+sin(x)−4=0

Solution

NoSolutionforx∈R
Solution steps
sin3(x)+sin(x)−4=0
Solve by substitution
sin3(x)+sin(x)−4=0
Let: sin(x)=uu3+u−4=0
u3+u−4=0:u≈1.37879…
u3+u−4=0
Find one solution for u3+u−4=0 using Newton-Raphson:u≈1.37879…
u3+u−4=0
Newton-Raphson Approximation Definition
f(u)=u3+u−4
Find f′(u):3u2+1
dud​(u3+u−4)
Apply the Sum/Difference Rule: (f±g)′=f′±g′=dud​(u3)+dudu​−dud​(4)
dud​(u3)=3u2
dud​(u3)
Apply the Power Rule: dxd​(xa)=a⋅xa−1=3u3−1
Simplify=3u2
dudu​=1
dudu​
Apply the common derivative: dudu​=1=1
dud​(4)=0
dud​(4)
Derivative of a constant: dxd​(a)=0=0
=3u2+1−0
Simplify=3u2+1
Let u0​=4Compute un+1​ until Δun+1​<0.000001
u1​=2.69387…:Δu1​=1.30612…
f(u0​)=43+4−4=64f′(u0​)=3⋅42+1=49u1​=2.69387…
Δu1​=∣2.69387…−4∣=1.30612…Δu1​=1.30612…
u2​=1.89271…:Δu2​=0.80116…
f(u1​)=2.69387…3+2.69387…−4=18.24328…f′(u1​)=3⋅2.69387…2+1=22.77092…u2​=1.89271…
Δu2​=∣1.89271…−2.69387…∣=0.80116…Δu2​=0.80116…
u3​=1.49490…:Δu3​=0.39780…
f(u2​)=1.89271…3+1.89271…−4=4.67308…f′(u2​)=3⋅1.89271…2+1=11.74707…u3​=1.49490…
Δu3​=∣1.49490…−1.89271…∣=0.39780…Δu3​=0.39780…
u4​=1.38644…:Δu4​=0.10846…
f(u3​)=1.49490…3+1.49490…−4=0.83561…f′(u3​)=3⋅1.49490…2+1=7.70421…u4​=1.38644…
Δu4​=∣1.38644…−1.49490…∣=0.10846…Δu4​=0.10846…
u5​=1.37883…:Δu5​=0.00760…
f(u4​)=1.38644…3+1.38644…−4=0.05148…f′(u4​)=3⋅1.38644…2+1=6.76665…u5​=1.37883…
Δu5​=∣1.37883…−1.38644…∣=0.00760…Δu5​=0.00760…
u6​=1.37879…:Δu6​=0.00003…
f(u5​)=1.37883…3+1.37883…−4=0.00024…f′(u5​)=3⋅1.37883…2+1=6.70353…u6​=1.37879…
Δu6​=∣1.37879…−1.37883…∣=0.00003…Δu6​=0.00003…
u7​=1.37879…:Δu7​=7.93136E−10
f(u6​)=1.37879…3+1.37879…−4=5.31658E−9f′(u6​)=3⋅1.37879…2+1=6.70324…u7​=1.37879…
Δu7​=∣1.37879…−1.37879…∣=7.93136E−10Δu7​=7.93136E−10
u≈1.37879…
Apply long division:u−1.37879…u3+u−4​=u2+1.37879…u+2.90108…
u2+1.37879…u+2.90108…≈0
Find one solution for u2+1.37879…u+2.90108…=0 using Newton-Raphson:No Solution for u∈R
u2+1.37879…u+2.90108…=0
Newton-Raphson Approximation Definition
f(u)=u2+1.37879…u+2.90108…
Find f′(u):2u+1.37879…
dud​(u2+1.37879…u+2.90108…)
Apply the Sum/Difference Rule: (f±g)′=f′±g′=dud​(u2)+dud​(1.37879…u)+dud​(2.90108…)
dud​(u2)=2u
dud​(u2)
Apply the Power Rule: dxd​(xa)=a⋅xa−1=2u2−1
Simplify=2u
dud​(1.37879…u)=1.37879…
dud​(1.37879…u)
Take the constant out: (a⋅f)′=a⋅f′=1.37879…dudu​
Apply the common derivative: dudu​=1=1.37879…⋅1
Simplify=1.37879…
dud​(2.90108…)=0
dud​(2.90108…)
Derivative of a constant: dxd​(a)=0=0
=2u+1.37879…+0
Simplify=2u+1.37879…
Let u0​=−2Compute un+1​ until Δun+1​<0.000001
u1​=−0.41924…:Δu1​=1.58075…
f(u0​)=(−2)2+1.37879…(−2)+2.90108…=4.14348…f′(u0​)=2(−2)+1.37879…=−2.62120…u1​=−0.41924…
Δu1​=∣−0.41924…−(−2)∣=1.58075…Δu1​=1.58075…
u2​=−5.04396…:Δu2​=4.62472…
f(u1​)=(−0.41924…)2+1.37879…(−0.41924…)+2.90108…=2.49879…f′(u1​)=2(−0.41924…)+1.37879…=0.54031…u2​=−5.04396…
Δu2​=∣−5.04396…−(−0.41924…)∣=4.62472…Δu2​=4.62472…
u3​=−2.58814…:Δu3​=2.45582…
f(u2​)=(−5.04396…)2+1.37879…(−5.04396…)+2.90108…=21.38809…f′(u2​)=2(−5.04396…)+1.37879…=−8.70914…u3​=−2.58814…
Δu3​=∣−2.58814…−(−5.04396…)∣=2.45582…Δu3​=2.45582…
u4​=−0.99998…:Δu4​=1.58816…
f(u3​)=(−2.58814…)2+1.37879…(−2.58814…)+2.90108…=6.03105…f′(u3​)=2(−2.58814…)+1.37879…=−3.79749…u4​=−0.99998…
Δu4​=∣−0.99998…−(−2.58814…)∣=1.58816…Δu4​=1.58816…
u5​=3.06056…:Δu5​=4.06054…
f(u4​)=(−0.99998…)2+1.37879…(−0.99998…)+2.90108…=2.52227…f′(u4​)=2(−0.99998…)+1.37879…=−0.62116…u5​=3.06056…
Δu5​=∣3.06056…−(−0.99998…)∣=4.06054…Δu5​=4.06054…
u6​=0.86213…:Δu6​=2.19842…
f(u5​)=3.06056…2+1.37879…⋅3.06056…+2.90108…=16.48802…f′(u5​)=2⋅3.06056…+1.37879…=7.49992…u6​=0.86213…
Δu6​=∣0.86213…−3.06056…∣=2.19842…Δu6​=2.19842…
u7​=−0.69537…:Δu7​=1.55751…
f(u6​)=0.86213…2+1.37879…⋅0.86213…+2.90108…=4.83307…f′(u6​)=2⋅0.86213…+1.37879…=3.10307…u7​=−0.69537…
Δu7​=∣−0.69537…−0.86213…∣=1.55751…Δu7​=1.55751…
u8​=202.24500…:Δu8​=202.94037…
f(u7​)=(−0.69537…)2+1.37879…(−0.69537…)+2.90108…=2.42584…f′(u7​)=2(−0.69537…)+1.37879…=−0.01195…u8​=202.24500…
Δu8​=∣202.24500…−(−0.69537…)∣=202.94037…Δu8​=202.94037…
u9​=100.77182…:Δu9​=101.47317…
f(u8​)=202.24500…2+1.37879…⋅202.24500…+2.90108…=41184.79638…f′(u8​)=2⋅202.24500…+1.37879…=405.86879…u9​=100.77182…
Δu9​=∣100.77182…−202.24500…∣=101.47317…Δu9​=101.47317…
u10​=50.02925…:Δu10​=50.74256…
f(u9​)=100.77182…2+1.37879…⋅100.77182…+2.90108…=10296.80558…f′(u9​)=2⋅100.77182…+1.37879…=202.92244…u10​=50.02925…
Δu10​=∣50.02925…−100.77182…∣=50.74256…Δu10​=50.74256…
u11​=24.64601…:Δu11​=25.38324…
f(u10​)=50.02925…2+1.37879…⋅50.02925…+2.90108…=2574.80799…f′(u10​)=2⋅50.02925…+1.37879…=101.43731…u11​=24.64601…
Δu11​=∣24.64601…−50.02925…∣=25.38324…Δu11​=25.38324…
u12​=11.93043…:Δu12​=12.71558…
f(u11​)=24.64601…2+1.37879…⋅24.64601…+2.90108…=644.30902…f′(u11​)=2⋅24.64601…+1.37879…=50.67082…u12​=11.93043…
Δu12​=∣11.93043…−24.64601…∣=12.71558…Δu12​=12.71558…
u13​=5.52440…:Δu13​=6.40602…
f(u12​)=11.93043…2+1.37879…⋅11.93043…+2.90108…=161.68600…f′(u12​)=2⋅11.93043…+1.37879…=25.23966…u13​=5.52440…
Δu13​=∣5.52440…−11.93043…∣=6.40602…Δu13​=6.40602…
u14​=2.22230…:Δu14​=3.30209…
f(u13​)=5.52440…2+1.37879…⋅5.52440…+2.90108…=41.03718…f′(u13​)=2⋅5.52440…+1.37879…=12.42761…u14​=2.22230…
Δu14​=∣2.22230…−5.52440…∣=3.30209…Δu14​=3.30209…
u15​=0.34989…:Δu15​=1.87241…
f(u14​)=2.22230…2+1.37879…⋅2.22230…+2.90108…=10.90385…f′(u14​)=2⋅2.22230…+1.37879…=5.82341…u15​=0.34989…
Δu15​=∣0.34989…−2.22230…∣=1.87241…Δu15​=1.87241…
u16​=−1.33680…:Δu16​=1.68669…
f(u15​)=0.34989…2+1.37879…⋅0.34989…+2.90108…=3.50593…f′(u15​)=2⋅0.34989…+1.37879…=2.07858…u16​=−1.33680…
Δu16​=∣−1.33680…−0.34989…∣=1.68669…Δu16​=1.68669…
u17​=0.86039…:Δu17​=2.19719…
f(u16​)=(−1.33680…)2+1.37879…(−1.33680…)+2.90108…=2.84494…f′(u16​)=2(−1.33680…)+1.37879…=−1.29480…u17​=0.86039…
Δu17​=∣0.86039…−(−1.33680…)∣=2.19719…Δu17​=2.19719…
Cannot find solution
The solution isu≈1.37879…
Substitute back u=sin(x)sin(x)≈1.37879…
sin(x)≈1.37879…
sin(x)=1.37879…:No Solution
sin(x)=1.37879…
−1≤sin(x)≤1NoSolution
Combine all the solutionsNoSolutionforx∈R

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Frequently Asked Questions (FAQ)

  • What is the general solution for sin^3(x)+sin(x)-4=0 ?

    The general solution for sin^3(x)+sin(x)-4=0 is No Solution for x\in\mathbb{R}
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