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Physics Helpline
L K Satapathy Laws of Motion 7
Pulley Block System
2M M
Physics Helpline
L K Satapathy Laws of Motion 7
Question : Two blocks of masses M and 2M are connected by a
metal wire of cross sectional area passing over a light
smooth pulley as shown in the figure . The breaking stress of the wire
is . The system is released from rest . The maximum
value of M for which the wire will not break is [Take ]
( ) 2 ( ) 4 ( ) 6 ( ) 8a kg b kg c kg d kg
Answer :
9 2
2 10 .N m

8 2
4 10 m

2M M
Let the common acceleration of the system = a
 The block of mass 2M will move down with acceleration a
& The block of mass M will move up with acceleration a
Tension in the wire should not exceed the breaking force of the wire
2
10g m s
Physics Helpline
L K Satapathy Laws of Motion 7
Let the tension in the wire = T
Mg
T
a M
(i) For mass 2M :
2Mg
T
a 2M
2 2 . . . (1)Mg T Ma 
(ii) For mass M : . . . (2)T Mg Ma 
To find T : We multiply equation (2) by 2
2 2 2 . . . (3)T Mg Ma  
(3) (1) (2 2 ) (2 ) 0T Mg Mg T     
3 4 0T Mg  
4
3
Mg
T 
We can also use
1 2
1 2
1 2
2
2 ,
m m g
T
m m
m M m M


 
[Free body diagram]
Physics Helpline
L K Satapathy Laws of Motion 7
[6 ]M kg Ans 
Correct option = (c)
Breaking stress of the wire = 9 2
2 10 .N m

Cross sectional area of the wire = 8 2
4 10 m

Breaking force of the wire = 9 2 8 2
(2 10 . )(4 10 ) 80N m m N 
  
 Tension in the wire should be  80N
In the limiting case , T = 80N
4
80
3
Mg
 
40
80
3
M
 
2
10g m s  
Physics Helpline
L K Satapathy
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Laws of Motion QA 7

  • 1. Physics Helpline L K Satapathy Laws of Motion 7 Pulley Block System 2M M
  • 2. Physics Helpline L K Satapathy Laws of Motion 7 Question : Two blocks of masses M and 2M are connected by a metal wire of cross sectional area passing over a light smooth pulley as shown in the figure . The breaking stress of the wire is . The system is released from rest . The maximum value of M for which the wire will not break is [Take ] ( ) 2 ( ) 4 ( ) 6 ( ) 8a kg b kg c kg d kg Answer : 9 2 2 10 .N m  8 2 4 10 m  2M M Let the common acceleration of the system = a  The block of mass 2M will move down with acceleration a & The block of mass M will move up with acceleration a Tension in the wire should not exceed the breaking force of the wire 2 10g m s
  • 3. Physics Helpline L K Satapathy Laws of Motion 7 Let the tension in the wire = T Mg T a M (i) For mass 2M : 2Mg T a 2M 2 2 . . . (1)Mg T Ma  (ii) For mass M : . . . (2)T Mg Ma  To find T : We multiply equation (2) by 2 2 2 2 . . . (3)T Mg Ma   (3) (1) (2 2 ) (2 ) 0T Mg Mg T      3 4 0T Mg   4 3 Mg T  We can also use 1 2 1 2 1 2 2 2 , m m g T m m m M m M     [Free body diagram]
  • 4. Physics Helpline L K Satapathy Laws of Motion 7 [6 ]M kg Ans  Correct option = (c) Breaking stress of the wire = 9 2 2 10 .N m  Cross sectional area of the wire = 8 2 4 10 m  Breaking force of the wire = 9 2 8 2 (2 10 . )(4 10 ) 80N m m N      Tension in the wire should be  80N In the limiting case , T = 80N 4 80 3 Mg   40 80 3 M   2 10g m s  
  • 5. Physics Helpline L K Satapathy For More details: www.physics-helpline.com Subscribe our channel: youtube.com/physics-helpline Follow us on Facebook and Twitter: facebook.com/physics-helpline twitter.com/physics-helpline