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Question

Question: How do you solve \[\sin (2t) + \sin (t) = 0\]?...

How do you solve sin(2t)+sin(t)=0\sin (2t) + \sin (t) = 0?

Explanation

Solution

First, we know that double angle identities are special cases of the sum identities. That is, when the two angles are equal, the sum identities are reduced to double angle identities.
The double sine formula is,
sin2A=2sinAcosA\sin 2A = 2\sin A\cos A
We will substitute this double angle formula in the given equation. Then, we will take sin common and keep each factor equal to 0.
After we solve for cost\cos t and find the value of tt
And finally, we will find the value of tt.
sint\sin t will repeat after every pie, so we find π\pi and 2π2\pi .

Complete step-by-step solution:
The given equation is, sin(2t)+sin(t)=0\sin (2t) + \sin (t) = 0
We know thatsin2A=2sinAcosA\sin 2A = 2\sin A\cos A .
Convert AA into tt, hence we get,
sin(2t)=2sintcost\Rightarrow \sin (2t) = 2\sin t\cos t
Putting this in the given equation,
2sintcost+sint=0\Rightarrow 2\sin t\cos t + \sin t = 0
Now we will take sint\sin t common in LHS (Left Hand Side), hence we get
sint(2cost+1)=0\Rightarrow \sin t(2\cos t + 1) = 0
If any individual factor on the left side of the equation is equal to 00, the entire expression will be equal to 00.
We separate the sine and cosine, we get
sint=0\Rightarrow \sin t = 0 or
2cost+1=0\Rightarrow 2\cos t + 1 = 0
Now we will find the value of cost\cos t, interchange LHS to RHS, we get
2cost=1\Rightarrow 2\cos t = - 1
Dividing by 22 on both sides, we get
cost=12\Rightarrow \cos t = - \dfrac{1}{2}
Now find the value of tt
t=cos1(12)\Rightarrow t = co{s^{ - 1}}\left( { - \dfrac{1}{2}} \right)
The exact value of cos1(12)co{s^{ - 1}}\left( { - \dfrac{1}{2}} \right) is 2π3\dfrac{{2\pi }}{3} and it can also be 4π3\dfrac{{4\pi }}{3} .
Since we are not given any range within which our tt lies, we will have to find a general solution.
If cosθ=cosβ\cos \theta = \cos \beta , then θ=2nπ+β\theta = 2n\pi + \beta . Using this, we get,
t=2nπ+2π3t = 2n\pi + \dfrac{{2\pi }}{3} and t=2nπ+4π3t = 2n\pi + \dfrac{{4\pi }}{3}
Now, set the first factor equal to 00.
sint=0\Rightarrow \sin t = 0
Take the inverse function of both sides of the equation to extract tt from inside the sine
t=sin1(0)\Rightarrow t = si{n^{ - 1}}(0)
The exact value of sin1(0)si{n^{ - 1}}(0) is 00 but it can also be π\pi . Since we are not given any range within which our t lies, we will have to find a general solution.
If sinθ=sinα\sin \theta = \sin \alpha , then, θ=nπ+α\theta = n\pi + \alpha . Using this,
sint=0=sin0\sin t = 0 = \sin 0^\circ , t=nπ+0=nπt = n\pi + 0 = n\pi .
Therefore, we have got the required values as nπ,2nπ+2π3,2nπ+4π3n\pi ,2n\pi + \dfrac{{2\pi }}{3},2n\pi + \dfrac{{4\pi }}{3} .
The final solution is all the values that make,
t=2πn,π+2πn,2π3+2πn,4π3+2πn\Rightarrow t = 2\pi n,\pi + 2\pi n,\dfrac{{2\pi }}{3} + 2\pi n,\dfrac{{4\pi }}{3} + 2\pi n, for any integernn.
Consolidate 2πn2\pi n and π+2πn\pi + 2\pi n to πn\pi n

t=πn,2π3+2πn,4π3+2πn t = \pi n,\dfrac{{2\pi }}{3} + 2\pi n,\dfrac{{4\pi }}{3} + 2\pi n , for any integer nn.

Note: Application of sin2A=2sinAcosA\sin 2A = 2\sin A\cos A: When an object is projected with speed uu at an angle α\alpha to the horizontal over level, the horizontal distance (Range) it travels before striking the ground is given by the formula
R=u2sin2αgR = \dfrac{{{u^2}\sin 2\alpha }}{g}
Clearly maximum of RR is u2g\dfrac{{{u^2}}}{g}, whenα=π4\alpha = \dfrac{\pi }{4}