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Joint Entrance Examination
Mathematics
Indefinite Integrals
Question 399
Question 399 of 416
Hard
MCQ
If \[\int {{1 \over x}\sqrt {{{1 - x} \over {1 + x}}} dx = g(x) + c} \],
g
(
1
)
=
0
g(1) = 0
g
(
1
)
=
0
, then \[g\left( {{1 \over 2}} \right)\] is equal to :
A
\[{\log _e}\left( {{{\sqrt 3 - 1} \over {\sqrt 3 + 1}}} \right) + {\pi \over 3}\]
B
\[{\log _e}\left( {{{\sqrt 3 + 1} \over {\sqrt 3 - 1}}} \right) + {\pi \over 3}\]
C
\[{\log _e}\left( {{{\sqrt 3 + 1} \over {\sqrt 3 - 1}}} \right) - {\pi \over 3}\]
D
\[{1 \over 2}{\log _e}\left( {{{\sqrt 3 - 1} \over {\sqrt 3 + 1}}} \right) - {\pi \over 6}\]
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Official solution
Given, \[\int {{1 \over x}\sqrt {{{1 - x} \over {1 + x}}} dx = g(x) + c} \],
g
(
1
)
=
0
g(1) = 0
g
(
1
)
=
0
Let I =
∫
1
x
1
−
x
1
+
x
d
x
\int {{1 \over x}\sqrt {{{1 - x} \over {1 + x}}} dx}
∫
x
1
1
+
x
1
−
x
d
x
=
∫
1
x
(
1
−
x
)
(
1
+
x
)
(
1
+
x
)
(
1
+
x
)
d
x
\int {{1 \over x}\sqrt {{{\left( {1 - x} \right)\left( {1 + x} \right)} \over {\left( {1 + x} \right)\left( {1 + x} \right)}}} } dx
∫
x
1
(
1
+
x
)
(
1
+
x
)
(
1
−
x
)
(
1
+
x
)
d
x
=
∫
1
−
x
x
1
−
x
2
d
x
=\int \frac{1-x}{x \sqrt{1-x^2}} d x
=
∫
x
1
−
x
2
1
−
x
d
x
=
∫
1
x
1
−
x
2
d
x
−
∫
1
1
−
x
2
d
x
=\int \frac{1}{x \sqrt{1-x^2}} d x-\int \frac{1}{\sqrt{1-x^2}} d x
=
∫
x
1
−
x
2
1
d
x
−
∫
1
−
x
2
1
d
x
Put
x
=
1
t
x=\frac{1}{t}
x
=
t
1
d
x
=
−
1
t
2
d x=-\frac{1}{t^2}
d
x
=
−
t
2
1
=
∫
−
1
t
2
1
t
1
−
1
t
2
d
t
−
sin
−
1
(
x
)
+
C
1
=\int \frac{\frac{-1}{t^2}}{\frac{1}{t} \sqrt{1-\frac{1}{t^2}}} d t-\sin ^{-1}(x)+C_1
=
∫
t
1
1
−
t
2
1
t
2
−
1
d
t
−
sin
−
1
(
x
)
+
C
1
=
∫
−
d
t
t
2
−
1
−
sin
−
1
(
x
)
+
C
1
=\int \frac{-d t}{\sqrt{t^2-1}}-\sin ^{-1}(x)+C_1
=
∫
t
2
−
1
−
d
t
−
sin
−
1
(
x
)
+
C
1
=
−
ln
∣
t
+
t
2
−
1
∣
−
sin
−
1
(
x
)
+
C
1
=-\ln \left|t+\sqrt{t^2-1}\right|-\sin ^{-1}(x)+C_1
=
−
ln
t
+
t
2
−
1
−
sin
−
1
(
x
)
+
C
1
=
−
ln
∣
1
x
+
1
x
2
−
1
∣
−
sin
−
1
(
x
)
+
C
1
=-\ln \left|\frac{1}{\mathrm{x}}+\sqrt{\frac{1}{\mathrm{x}^2}-1}\right|-\sin ^{-1}(\mathrm{x})+\mathrm{C}_1
=
−
ln
x
1
+
x
2
1
−
1
−
sin
−
1
(
x
)
+
C
1
[Putting values of t]
=
−
ln
∣
1
x
+
1
x
2
−
1
∣
−
(
π
2
−
cos
−
1
x
)
+
C
1
=-\ln \left|\frac{1}{\mathrm{x}}+\sqrt{\frac{1}{\mathrm{x}^2}-1}\right|-\left(\frac{\pi}{2}-\cos ^{-1} \mathrm{x}\right)+\mathrm{C}_1
=
−
ln
x
1
+
x
2
1
−
1
−
(
2
π
−
cos
−
1
x
)
+
C
1
=
−
ln
∣
1
x
+
1
x
2
−
1
∣
+
cos
−
1
(
x
)
−
π
2
+
C
1
=-\ln \left|\frac{1}{\mathrm{x}}+\sqrt{\frac{1}{\mathrm{x}^2}-1}\right|+\cos ^{-1}(\mathrm{x})-\frac{\pi}{2}+\mathrm{C}_1
=
−
ln
x
1
+
x
2
1
−
1
+
cos
−
1
(
x
)
−
2
π
+
C
1
\[ \therefore \]
g
(
x
)
=
cos
−
1
(
x
)
−
ℓ
n
∣
1
x
+
1
x
2
−
1
∣
g(x)=\cos ^{-1}(x)-\ell n\left|\frac{1}{x}+\sqrt{\frac{1}{x^2}-1}\right|
g
(
x
)
=
cos
−
1
(
x
)
−
ℓ
n
x
1
+
x
2
1
−
1
So,
g
(
1
)
=
cos
−
1
(
1
)
−
ℓ
n
∣
1
∣
=
0
g(1)=\cos ^{-1}(1)-\ell n|1|=0
g
(
1
)
=
cos
−
1
(
1
)
−
ℓ
n
∣1∣
=
0
g
(
1
2
)
=
cos
−
1
(
1
2
)
−
ℓ
n
∣
2
+
3
∣
g\left(\frac{1}{2}\right)=\cos ^{-1}\left(\frac{1}{2}\right)-\ell n|2+\sqrt{3}|
g
(
2
1
)
=
cos
−
1
(
2
1
)
−
ℓ
n
∣2
+
3
∣
=
π
3
+
ln
(
1
2
+
3
)
= {\pi \over 3} + \ln \left( {{1 \over {2 + \sqrt 3 }}} \right)
=
3
π
+
ln
(
2
+
3
1
)
=
π
3
+
ln
(
3
−
1
3
+
1
)
=\frac{\pi}{3}+\ln \left(\frac{\sqrt{3}-1}{\sqrt{3}+1}\right)
=
3
π
+
ln
(
3
+
1
3
−
1
)
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