1) The inextensible string: i.c if M moves a distance x then m moves the same distance x and therefore M and m have the same speed and the same lincar acceleration. R 2) The mass M is under the action of its weight Mg, the reaction of the support M T. 4. R and the tension of the string Applying Newton's second law on M:Fet =Ma Mg+T+R =Ma Mg Projecting this relation on a horizontal axis parallel and in the same direction of the motion of M: 0+T+0= Ma T= Ma The mass m is under the action of its weight mg and the tension of the string t. Applying Newton's second law on m : Fext = ma =mg+ t ma -> mg Projecting this relation on the vertically downward axis : mg -t = ma t =m(g-a)| 3) The pulley is under the action of its weight ug, the reaction R' of the axis of R' rotation (A) and of tensions T' and t' of the string on the pulley. Applying Newton's second law for rotation on the pulley: = 10" Fat/(A) + M. + M, = 10" u g/(A) R/ T/(A) t'/(A) -T'r t'r =0 since u g intersects with (A) =0 since R' intersects with (A) 10" =-T'r+t'r = 10" => t'-T' =- But the string is of negligible mass, hence the tension of the string is constant. : t' =t and T'= T

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N° 11
Complex motion (2)
1) The inextensible string: i.c if M moves a distance x then m moves the same distance x and therefore
M and m have the same speed and the same linear acceleration.
R
2) The mass M is under the action of its weight Mg, the reaction of the support
M
4.
R and the tension of the string T.
Applying Newton's second law on M:
EFeu =Ma = Mg+T+R =Ma
Mg
Projecting this relation on a horizontal axis parallel and in the same direction of
the motion of M: 0+T+0= Ma T=Ma
The mass m is under the action of its weight mg and the tension of the string t
1.
m
Applying Newton's second law on m:
ext = ma = mg+t = m a
mg
Projecting this relation on the vertically downward axis :
mg -t = ma =t =m(g-a)|.
3) The pulley is under the action of its weight u g, the reaction R' of the axis of
rotation (A) and of tensions T' and t' of the string on the pulley.
Applying Newton's second law for rotation on the pulley:
= 10"
Fat/(A)
+ M,
= 10"
u g/(A)
R/(A)
T'/(A)
t'/(A)
-T'.r
t'r
=0 since u g intersects with (A)
=0 since R'intersects with (A)
10"
=-T'r+t'r = 10" > t'-T' =-
But the string is of negligible mass, hence the tension of the string is constant. :
t' =t and T'= T
Transcribed Image Text:N° 11 Complex motion (2) 1) The inextensible string: i.c if M moves a distance x then m moves the same distance x and therefore M and m have the same speed and the same linear acceleration. R 2) The mass M is under the action of its weight Mg, the reaction of the support M 4. R and the tension of the string T. Applying Newton's second law on M: EFeu =Ma = Mg+T+R =Ma Mg Projecting this relation on a horizontal axis parallel and in the same direction of the motion of M: 0+T+0= Ma T=Ma The mass m is under the action of its weight mg and the tension of the string t 1. m Applying Newton's second law on m: ext = ma = mg+t = m a mg Projecting this relation on the vertically downward axis : mg -t = ma =t =m(g-a)|. 3) The pulley is under the action of its weight u g, the reaction R' of the axis of rotation (A) and of tensions T' and t' of the string on the pulley. Applying Newton's second law for rotation on the pulley: = 10" Fat/(A) + M, = 10" u g/(A) R/(A) T'/(A) t'/(A) -T'.r t'r =0 since u g intersects with (A) =0 since R'intersects with (A) 10" =-T'r+t'r = 10" > t'-T' =- But the string is of negligible mass, hence the tension of the string is constant. : t' =t and T'= T
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