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Question: For \[0 < \phi < \dfrac{\pi }{2}\],if \[x = \sum\nolimits_{n = 0}^\infty {{{\cos }^{2n}}} \phi \], \...

For 0<ϕ<π20 < \phi < \dfrac{\pi }{2},if x=n=0cos2nϕx = \sum\nolimits_{n = 0}^\infty {{{\cos }^{2n}}} \phi , y=n=0sin2nϕy = \sum\nolimits_{n = 0}^\infty {{{\sin }^{2n}}} \phi and z=n=0cos2nϕsin2nϕz = \sum\nolimits_{n = 0}^\infty {{{\cos }^{2n}}} \phi {\sin ^{2n}}\phi then xyzxyz=
A) xy+zxy + z
B) xz+yxz + y
C) x+y+zx + y + z
D) yz+xyz + x

Explanation

Solution

In the given question, we are given that let 0<ϕ<π20 < \phi < \dfrac{\pi }{2} Also we are given the values of three variables xx, yy and zzin the terms of trigonometric terms or trigonometric ratios sinϕ\sin \phi and cosϕ\cos \phi with their powers up to nn and therefore we have to find out the relationship between xx, yy and zz.

Complete step-by-step answer:
In the given question, we are given the range of angle ϕ\phi which is 0<ϕ<π20 < \phi < \dfrac{\pi }{2} Also we are given the values of three variables xx, yy and zzin terms of n and 2n2n powers of trigonometric ratios cosϕ\cos \phi and sinϕ\sin \phi . Therefore using various trigonometric identities we will find out the relationship between these three variables xx, yy and zz. Firstly we are going to solve the values of x,y,zx,y,z.
On solving xx, we get
Given x=n=0cos2nϕx = \sum\limits_{n = 0}^\infty {{{\cos }^{2n}}} \phi
On substituting the values of n=0n = 0to n=n = \infty and then summing all the terms because of (MISSING A SIGN)
Therefore we get,
x=cos2(0)ϕ+cos2(1)ϕ+cos2(2)ϕ+.........x = {\cos ^{2(0)}}\phi + {\cos ^{2(1)}}\phi + {\cos ^{2(2)}}\phi + .........\infty
x=cos0ϕ+cos2ϕ+cos4ϕ+.........x = {\cos ^0}\phi + {\cos ^2}\phi + {\cos ^4}\phi + .........\infty
Here, using T-ratios formulas, we know, the values of cos0ϕ=1{\cos ^0}\phi = 1
Therefore on substituting, we get
x=1+cos2ϕ+cos4ϕ+.............x = 1 + {\cos ^2}\phi + {\cos ^4}\phi + .............\infty
This is geometric progression with first term (a) = 1\left( a \right){\text{ }} = {\text{ }}1and common ratio (r)=cos2ϕ1=cos2ϕ\left( r \right) = \dfrac{{{{\cos }^2}\phi }}{1} = {\cos ^2}\phi . Therefore sum of geometric progression ua1ru\dfrac{a}{{1 - r}}
x=11cos2ϕx = \dfrac{1}{{1 - {{\cos }^2}\phi }}
because a=1a = 1& r=cos2ϕr = {\cos ^2}\phi
Also, cos2ϕ+sin2ϕ=1{\cos ^2}\phi + {\sin ^2}\phi = 1 which implies cos2ϕ=1sin2ϕ{\cos ^2}\phi = 1 - {\sin ^2}\phi
Therefore = 11(1sin2ϕ)=111+sin2ϕ=1sin2ϕ\dfrac{1}{{1 - (1 - {{\sin }^2}\phi )}} = \dfrac{1}{{1 - 1 + {{\sin }^2}\phi }} = \dfrac{1}{{{{\sin }^2}\phi }}
x=1sin2ϕx = \dfrac{1}{{{{\sin }^2}\phi }}
On solving yy, we get
y=n=0sin2nϕy = \sum\limits_{n = 0}^\infty {{{\sin }^{2n}}\phi }
Putting values of n=1,2,3,.......n = 1,2,3,.......\infty and summing, we get
y=sin2(0)ϕ+sin2(1)ϕ+sin2(2)ϕ+........y = {\sin ^{2(0)}}\phi + {\sin ^{2(1)}}\phi + {\sin ^{2(2)}}\phi + ........\infty
y=1+sin2ϕ+sin4ϕ+........y = 1 + {\sin ^2}\phi + {\sin ^4}\phi + ........\infty Y = ...
where sin0ϕ=1{\sin ^0}\phi = 1 and this becomes a geometric progression with a=1a = 1and r=sin2ϕr = {\sin ^2}\phi .
so, y=11sin2ϕ=1cos2ϕy = \dfrac{1}{{1 - {{\sin }^2}\phi }} = \dfrac{1}{{{{\cos }^2}\phi }}
because sin2ϕ+cos2ϕ=1{\sin ^2}\phi + {\cos ^2}\phi = 1 which implies 1sin2ϕ=cos2ϕ1 - {\sin ^2}\phi = {\cos ^2}\phi .
y=1cos2ϕy = \dfrac{1}{{{{\cos }^2}\phi }}
Also, on solving zz, we get
z=n=0cos2ϕsin2ϕz = \sum\limits_{n = 0}^\infty {{{\cos }^2}\phi } {\sin ^2}\phi
On putting n=0n = 0to \infty and summing, we get
z=cos2(0)ϕsin2(0)ϕ+cos2(1)ϕsin2(1)ϕ+cos2(2)ϕsin2(2)ϕ+........z = {\cos ^{2(0)}}\phi {\sin ^{2(0)}}\phi + {\cos ^{2(1)}}\phi {\sin ^{2(1)}}\phi + {\cos ^{2(2)}}\phi {\sin ^{2(2)}}\phi + ........\infty
z=1+cos2(1)ϕsin2(1)ϕ+cos2(2)ϕsin2(2)ϕ+........z = 1 + {\cos ^{2(1)}}\phi {\sin ^{2(1)}}\phi + {\cos ^{2(2)}}\phi {\sin ^{2(2)}}\phi + ........\infty
Where cos0ϕsin0ϕ=1{\cos ^0}\phi {\sin ^0}\phi = 1 and this becomes
Progression with a=1a = 1 & r=cos2ϕsin2ϕr = {\cos ^2}\phi {\sin ^2}\phi
z=11cos2ϕsin2ϕz = \dfrac{1}{{1 - {{\cos }^2}\phi {{\sin }^2}\phi }}
We got three values of variables xx, yy and zz
Here, we have to find xyzxyzand on substituting the values of xx, yy and zz in xyzxyz we get
xyz=1sin2ϕ.1cos2ϕ.11cos2ϕsin2ϕxyz = \dfrac{1}{{{{\sin }^2}\phi }}.\dfrac{1}{{{{\cos }^2}\phi }}.\dfrac{1}{{1 - {{\cos }^2}\phi {{\sin }^2}\phi }}
xyz=1(sin2ϕcos2ϕ)(1sin2ϕcos2ϕ)xyz = \dfrac{1}{{({{\sin }^2}\phi {{\cos }^2}\phi )(1 - {{\sin }^2}\phi {{\cos }^2}\phi )}}
By multiplying the terms we get the above equation.
Here in the numerator, we will add and subtract the term sin2ϕcos2ϕ{\sin ^2}\phi {\cos ^2}\phi so we get
xyz=1sin2ϕcos2ϕ+sin2ϕcos2ϕ(sin2ϕcos2ϕ)(1sin2ϕcos2ϕ)xyz = \dfrac{{1 - {{\sin }^2}\phi {{\cos }^2}\phi + {{\sin }^2}\phi {{\cos }^2}\phi }}{{({{\sin }^2}\phi {{\cos }^2}\phi )(1 - {{\sin }^2}\phi {{\cos }^2}\phi )}}
On splitting the terms in numerator, we get
xyz=1sin2ϕcos2ϕ(sin2ϕcos2ϕ)(1sin2ϕcos2ϕ)+sin2ϕcos2ϕ(sin2ϕcos2ϕ)(1sin2ϕcos2ϕ)xyz = \dfrac{{1 - {{\sin }^2}\phi {{\cos }^2}\phi }}{{({{\sin }^2}\phi {{\cos }^2}\phi )(1 - {{\sin }^2}\phi {{\cos }^2}\phi )}} + \dfrac{{{{\sin }^2}\phi {{\cos }^2}\phi }}{{({{\sin }^2}\phi {{\cos }^2}\phi )(1 - {{\sin }^2}\phi {{\cos }^2}\phi )}}
On canceling the terms we get
xyz=1sin2ϕcos2ϕ+11sin2ϕcos2ϕxyz = \dfrac{1}{{{{\sin }^2}\phi {{\cos }^2}\phi }} + \dfrac{1}{{1 - {{\sin }^2}\phi {{\cos }^2}\phi }}
xyz=1sin2ϕ1cos2ϕ+1sin2ϕcos2ϕxyz = \dfrac{1}{{{{\sin }^2}\phi }}\dfrac{1}{{{{\cos }^2}\phi }} + \dfrac{1}{{{{\sin }^2}\phi {{\cos }^2}\phi }}
On substituting the values of x,y,zx,y,z in this we get
xyz=xy+zxyz = xy + z

So, the correct answer is “Option A”.

Note: In the above question, we had solved xx, yy and zz firstly by substituting values of nn from 0 to 0{\text{ }}to{\text{ }}\infty and then summing all the terms and then that becomes geometric progression with the common term and common ratio geometric progression is the series which is the summation of terms with one common multiple which on further divided get common ratio.