![]() |
VOOZH | about |
Solution:
We have,
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I = [(a2 + b2)/2][π/2]
I = π(a2 + b2)/4
Therefore, the value of is π(a2 + b2)/4.
Solution:
We have,
I =
I =
I =
I =
I =
I =
I =
I =
I = 2[sinπ/4 - cosπ/4 - 0 + 1]
I = 2[1/√2 - 1/√2 - 0 + 1]
I = 2 (1)
I = 2
Therefore, the value of is 2.
Solution:
We have,
I =
I =
I =
I =
I =
I =
I = 2√2[sinπ/4 - sin0]
I = 2√2[1/√2- sin0]
I = 2√2[1/√2]
I = 2
Therefore, the value of is 2.
Solution:
We have,
I =
By using integration by parts, we get,
I = x ∫sinxdx - ∫(∫sin x (1)dx)dx
I = -xcosx - ∫(∫sin xdx)dx
I = -xcosx + ∫cosxdx
I = -xcosx + sinx
So we get,
I =
I = [-π/2cosπ/2 + sinπ/2 + 0 - 0]
I = 0 + 1 + 0 – 0
I = 1
Therefore, the value of is 1.
Solution:
We have,
I =
By using integration by parts, we get,
I = x∫cosxdx - ∫(∫cos x (1)dx)dx
I = xsinx - ∫(∫cosxdx)dx
I = xsinx - ∫sinxdx
I = x sin x + cos x
So we get,
I =
I = [π/2sinπ/2 + cosπ/2 - 0 - cos0]
I = π/2 + 0 - 0 - 1
I = π/2 - 1
Therefore, the value of is π/2 - 1.
Solution:
We have,
I =
By using integration by parts, we get,
I = x2sinx - ∫(2x∫(cosx)dx)dx
I = x2sinx - ∫(2xsinx)dx
I = x2sinx - 2[-xcosx - ∫(1∫sinxdx)dx]
I = x2sinx - 2[-xcosx + ∫sinxdx]
I = x2sinx - 2[-xcosx + sinx]
I = x2sinx + 2xcosx - 2sinx
So we get,
I =
I = [(π/2)2sinπ/2 + 2(π/2)cosπ/2 - 2sinπ/2 - 0 - 0 + sin0]
I = [π2/4 + 0 - 2 - 0 - 0 + 0]
I = π2/4 - 2
Therefore, the value of is π2/4 - 2.
Solution:
We have,
I =
By using integration by parts, we get,
I = -x2cosx - ∫(2x∫sinxdx)dx
I = -x2cosx + ∫(2xcosx)dx
I = -x2cosx + 2[xsinx - ∫(∫cosxdx)dx]
I = -x2cosx + 2[xsinx - ∫sinxdx]
I = -x2cosx + 2[xsinx + cosx]
I = -x2cosx + 2xsinx + 2cosx
So we get,
I =
I = -(π/4)2cosπ/4 + 2π/4sinπ/4 + 2cosπ/4 + 0 - 0 - 2
I = -π2/16(1/ √2) + π/2(1/√2) + 2(1/√2) + 0 - 0 - 2
I = -π2/16√2 + π/2√2 + √2 - 2
Therefore, the value of is -π2/16√2 + π/2√2 + √2 - 2.
Solution:
We have,
I =
By using integration by parts, we get,
I = 1/2x2sin2x - ∫(2x∫cos2xdx)dx
I = 1/2x2sin2x - ∫(xsin2x)dx
I = 1/2x2sin2x - [-1/2xcos2x - ∫(∫sin2xdx)dx]
I = 1/2x2sin2x - [-1/2xcos2x + ∫1/2 cos2xdx]
I = 1/2x2sin2x - [-1/2xcos2x + 1/4sin2xdx]
I = 1/2x2sin2x + 1/2xcos2x - 1/4sin2xdx
So we get,
I =
I = [1/2(π2/4)sinπ + 1/2(π/2)cosπ - 0 - 0 - 0 + 0]
I = -π/4
Therefore, the value of is -π/4.
Solution:
We have,
I =
I =
I =
I =
By using integration by parts, we get,
I = 1/2[x3/3] + x2sin2x/2 - [x ∫sin2x - ∫(∫sin2xdx)dx]
I = 1/2[x3/3] + x2sin2x/2 + xcosx/2 - sin2x/4
So we get,
I =
I = [1/6[π3/8] + 0 + 0 - π/8]
I = π3/48 - π/8
Therefore, the value of is π3/48 - π/8.
Solution:
We have,
I =
By using integration by parts, we get,
I =
I = xlogx - ∫1dx
I = xlogx - x
So we get,
I =
I = 2log2 - 2 - log1 + 1
I = 2 log 2 – 1
Therefore, the value of is 2 log 2 – 1.
Solution:
We have,
I =
By using integration by parts, we get,
I =
I =
I =
I =
So we get,
I =
I = -log3/4 + log3 - log4 + log1/2 - log1 + log2
I = log3(1 - 1/4) - 2log2 + 0 - 0 + log2
I = 3/4log3 - log2
Therefore, the value of is 3/4log3 - log2.
Solution:
We have,
I =
I =
I =
By using integration by parts, we get,
I =
I = exlogx
So we get,
I =
I = eeloge - e1log1
I = ee (1) – 0
I = ee
Therefore, the value of is ee.
Solution:
We have,
I =
Let log x = t, so we have,
=> (1/x) dx = dt
Now, the lower limit is, x = 1
=> t = log x
=> t = log 1
=> t = 0
Also, the upper limit is, x = e
=> t = log x
=> t = log e
=> t = 1
So, the equation becomes,
I =
I =
I =
I = 1/2 - 0/2
I = 1/2
Therefore, the value of is 1/2.
Solution:
We have,
I =
I =
By using integration by parts, we get,
I =
I =
I =
I = x/logx
So we get,
I =
I =
I =
I = e2/2 - e
Therefore, the value of is e2/2 - e.
Solution:
We have,
I =
I =
I =
I =
I =
I =
I =
I = 1/2[3log2 - log4 + log3]
I = 1/2[3log2 - 2log2 + log3]
I = 1/2[log 2 - log 3]
I = 1/2[log6]
I = log6/2
Therefore, the value of is log6/2.
Solution:
We have,
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I = [1/5log6 + 3/√5tan-1(√5) - 1/5log1 - 3/√5tan-1(0)]
I = [1/5 log6 + 3√5 tan-1(√5) - 0 - 0]
I = 1/5 log6 + 3√5 tan-1(√5)
Therefore, the value of is 1/5 log6 + 3√5 tan-1(√5).
Solution:
We have,
I =
I =
I =
I =
I =
I =
Let x – 1/2 = t, so we have,
=> dx = dt
Now, the lower limit is, x = 0
=> t = x – 1/2
=> t = 0 – 1/2
=> t = 1/2
Also, the upper limit is, x = 2
=> t = x – 1/2
=> t = 2 – 1/2
=> t = 3/2
So, the equation becomes,
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
Therefore, the value of is .
Solution:
We have,
I =
I =
I =
I =
I =
I =
I =
I =
I = 4/2√7[tan-1(5/√7) - tan-1(1/√7)]
I = 2/√7[tan-1(5/√7) - tan-1(1/√7)]
Therefore, the value of is 2/√7[tan-1(5/√7) - tan-1(1/√7)].
Solution:
We have,
I =
Let x = sin2 t, so we have,
=> dx = 2 sin t cos t dt
Now, the lower limit is, x = 0
=> sin2 t = 0
=> sin t = 0
=> t = 0
Also, the upper limit is, x = 1
=> sin2 t = 1
=> sin t = 1
=> t = π/2
So, the equation becomes,
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I =
I = 1/4[π/2 - 0] - 1/16[sin2π - 0]
I = 1/4[π/2] - 1/16[0 - 0 ]
I = π/8
Therefore, the value of is π/8.
Solution:
We have,
I =
I =
I =
I =
I =
I = [sin-1(1/2) - sin-1(-1/2)]
I = π/6 -(-π/6)
I = π/6 + π/6
I = π/3
Therefore, the value of is π/3.
Question 43.
Solution:
We have,
I =
I =
I =
I =
I =
I =
I = [sin-1(2/2) - sin-1(-2/2)]
I = sin-11 - sin-1(-1)
I = π/2 - (-π/2)
I = π/2 + π/2
I = π
Therefore, the value of is π.
Solution:
We have,
I =
I =
I =
Let x + 1 = t, so we have,
=> dx = dt
Now, the lower limit is, x = –1
=> t = x + 1
=> t = – 1 + 1
=> t = 0
Also, the upper limit is, x = 1
=> t = x + 1
=> t = 1 + 1
=> t = 2
So, the equation becomes,
I =
I =
I = 1/2tan-12/2 - 1/2tan-10/2
I = 1/2tan-11 - 1/2tan-10
I = 1/2(π/4) - 0
I = π/8
Therefore, the value of is π/8.
This exercise typically covers: