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Physics Helpline
L K Satapathy
Indefinite Integrals 1
Physics Helpline
L K Satapathy
Indefinite Integrals - 1
4
cos 2 .I x dx Answer-1
2
4 2 2 1 cos4
cos 2 (cos 2 )
2
x
x x
 
   
 
1 1 1 1
cos4 cos8
4 2 8 8
x x   
21
(1 2cos4 cos 4 )
4
x x  
4 3 1 1
cos 2 cos4 cos8
8 2 8
x x x   
1 1 1 1 cos8
cos4
4 2 4 2
x
x
 
    
 
Power of cos x has to be removed by converting to multiple angle
2
[2cos 1 cos2 ]  
Physics Helpline
L K Satapathy
Indefinite Integrals - 1
3 1 1
cos4 cos8 .
8 2 8
x x dx
 
   
 

4
cos 2 .x dx 
3 1 1
cos4 . cos8 .
8 2 8
dx x dx x dx    
 
3 1 sin4 1 sin8
8 2 4 8 8
x x
x C
   
      
   
     
3 1 1
sin4 sin8
8 8 6
]
4
[x x x AnC s   
Physics Helpline
L K Satapathy
Indefinite Integrals - 1
Answer-2
4 2 2 2 2 2
tan tan (sec 1) tan .sec tanx x x x x x   
4
tan .I x dx 
2 2 2
tan .sec (sec 1)x x x  
2 2 2
tan .sec . sec .x x dx x dx dx    
4
tan .x dx 
1 2 3 [ ]I I I say  
2 2 2
tan .sec sec 1x x x  
We simplify the integrand as follows:
Physics Helpline
L K Satapathy
Indefinite Integrals - 1
Answer-2
4 3
1 2 3
1
tan . tan tan
3
[ ]x dx I I I x x x C Ans       
2 2
1 tan .sec .I x x dx 
2
tan sec .x t x dx dt  
3
2 3
1
1
t . tan
3 3
t
I dt x   
2
2 sec . tanI x dx x 
3I dx x 
We evaluate the integrals separately.
Substitution :
Physics Helpline
L K Satapathy
Indefinite Integrals - 1
Answer-3
2
cos2
.
(cos sin )
x
I dx
x x


2 2
2 2
cos2 cos sin
(cos sin ) (cos sin )
x x x
x x x x


 
2
(cos sin )(cos sin )
(cos sin )
x x x x
x x
 


(cos sin )
(cos sin )
x x
x x



We simplify the integrand as follows:
Physics Helpline
L K Satapathy
Indefinite Integrals - 1
Answer-3
(cos sin )
.
(sin cos )
x x
dx
x x


2
cos2
.
(cos sin )
x
I dx
x x


As the derivative of sinx + cosx = cosx – sinx
sin cosx x t 
cos sin
. log( )
sin cos
x x dt
dx t C
x x t

   
 
(cos sin ).x x dx dt 
2
cos2
. log(sin cos )
(cos sin
[ ]
)
x
I dx x x AnsC
x x
   

We substitute :
Putting back the value of t , we get
Differentiating we get
Physics Helpline
L K Satapathy
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Indefinite Integrals 1

  • 1. Physics Helpline L K Satapathy Indefinite Integrals 1
  • 2. Physics Helpline L K Satapathy Indefinite Integrals - 1 4 cos 2 .I x dx Answer-1 2 4 2 2 1 cos4 cos 2 (cos 2 ) 2 x x x         1 1 1 1 cos4 cos8 4 2 8 8 x x    21 (1 2cos4 cos 4 ) 4 x x   4 3 1 1 cos 2 cos4 cos8 8 2 8 x x x    1 1 1 1 cos8 cos4 4 2 4 2 x x          Power of cos x has to be removed by converting to multiple angle 2 [2cos 1 cos2 ]  
  • 3. Physics Helpline L K Satapathy Indefinite Integrals - 1 3 1 1 cos4 cos8 . 8 2 8 x x dx          4 cos 2 .x dx  3 1 1 cos4 . cos8 . 8 2 8 dx x dx x dx       3 1 sin4 1 sin8 8 2 4 8 8 x x x C                      3 1 1 sin4 sin8 8 8 6 ] 4 [x x x AnC s   
  • 4. Physics Helpline L K Satapathy Indefinite Integrals - 1 Answer-2 4 2 2 2 2 2 tan tan (sec 1) tan .sec tanx x x x x x    4 tan .I x dx  2 2 2 tan .sec (sec 1)x x x   2 2 2 tan .sec . sec .x x dx x dx dx     4 tan .x dx  1 2 3 [ ]I I I say   2 2 2 tan .sec sec 1x x x   We simplify the integrand as follows:
  • 5. Physics Helpline L K Satapathy Indefinite Integrals - 1 Answer-2 4 3 1 2 3 1 tan . tan tan 3 [ ]x dx I I I x x x C Ans        2 2 1 tan .sec .I x x dx  2 tan sec .x t x dx dt   3 2 3 1 1 t . tan 3 3 t I dt x    2 2 sec . tanI x dx x  3I dx x  We evaluate the integrals separately. Substitution :
  • 6. Physics Helpline L K Satapathy Indefinite Integrals - 1 Answer-3 2 cos2 . (cos sin ) x I dx x x   2 2 2 2 cos2 cos sin (cos sin ) (cos sin ) x x x x x x x     2 (cos sin )(cos sin ) (cos sin ) x x x x x x     (cos sin ) (cos sin ) x x x x    We simplify the integrand as follows:
  • 7. Physics Helpline L K Satapathy Indefinite Integrals - 1 Answer-3 (cos sin ) . (sin cos ) x x dx x x   2 cos2 . (cos sin ) x I dx x x   As the derivative of sinx + cosx = cosx – sinx sin cosx x t  cos sin . log( ) sin cos x x dt dx t C x x t        (cos sin ).x x dx dt  2 cos2 . log(sin cos ) (cos sin [ ] ) x I dx x x AnsC x x      We substitute : Putting back the value of t , we get Differentiating we get
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