I =
.....(1) I =
......(2) Adding (1) and (2) 2I =
I =
I =
=
=
=
I =
.....(1) I =
......(2) Adding (1) and (2) 2I =
I =
I =
=
=
=
I2 =
I2 =
I2 =
I2 = I1 -
Now apply IBP I2 = I1 -
Let (1 – x50) = t -50x49dx = dt I2 = I1 -
-
= I1 - 0 -
I2 = I1 -
I2 +
= I1
= I1 I2 =
I1 Given I2 = I1 =
=
=
=
= e2 4 - e 1 = 4e2 - e = e(4e - 1) Note :
= exf(x) + c
I =
...(1) x a + b - x I =
I =
.....(2) [As ƒ(x) = ƒ(a + b + 1 - x) ƒ(x + 1) = ƒ(a + b - x)] Adding (1) and (2) we get 2I =
I =
I =
I =
I =
Let x = t + 1 I =
=
= 5
= 5
= 0 Let e- = t 4t2 + 4t - 3 = 0 t =
e- =
=
2cot2 -
+ 4 = 0
= 0 2sin2 – 5sin + 2 = 0 (2sin – 1)(sin – 2) = 0 sin =
[ sin = 2 not possible] 1 =
and 2 =
as 1
2 I =
=
=
=
Let f(x) =
f'(x) =
=
fmax = f(1) fmin = f(2) f(1) =
=
=
f(2) =
=
So
ƒ(x) = a + bx + cx2
=
=
=
f(1) = a + b + c f(0) = a
By checking each option you have to find the solution.
=
=
Option (A) is correct option.
F'(x) = x2g(x) = x2
F'(1) = (1)(0) = 0 Now, F''(x) = 2xg(x) + x2g'(x) F''(1) = 2g(1) + g'(1) = 0 + g'(1) = 3 [ As g'(t) = f(t); g'(1) = f'(1) = 3 ] So, at x = 1, F'(1) = 0 and F"(1) = 3 > 0 For the function f(x), x = 1 is a point of local minima.
This is in
form. So apply newton leibniz rule
= 0