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Assuming the string to have a uniform mass distribution and the external force to act along the length of a string, following procedure can be adopted.......
Due to applied force, the rope will accelerate over the smooth horizontal surface at the rate of given by
a=F/M
If we further assume that the rope is almost inextensible or non-deformable, it is obvious that acceleration of each small constituiting parts of the rope would be same and equal to a=F/M
Lets think by dividing the rope into two sections 1 and 2 as depicted in the picture above.Let T be the tension at the junction.We have now to analyse the dynamics of one of the two sections Consider the section 2
Mass of section 2 is
m2=(M/L)*(L-l)
Applying newton 's second law of motion on section 2,
T=m2a
or,T=(M/L)*(L-l)*(F/M)
or,T=(F/L)*(L-l)
In this way, we get tension as a function of l.
Also on putting y= 0 in above expression, we get tension at right equal angle to F and similarly on putting y=L, we get tension at left and equal to zero which are quite obvious results.
Hope you like it....
Mark as brainliest....
Due to applied force, the rope will accelerate over the smooth horizontal surface at the rate of given by
a=F/M
If we further assume that the rope is almost inextensible or non-deformable, it is obvious that acceleration of each small constituiting parts of the rope would be same and equal to a=F/M
Lets think by dividing the rope into two sections 1 and 2 as depicted in the picture above.Let T be the tension at the junction.We have now to analyse the dynamics of one of the two sections Consider the section 2
Mass of section 2 is
m2=(M/L)*(L-l)
Applying newton 's second law of motion on section 2,
T=m2a
or,T=(M/L)*(L-l)*(F/M)
or,T=(F/L)*(L-l)
In this way, we get tension as a function of l.
Also on putting y= 0 in above expression, we get tension at right equal angle to F and similarly on putting y=L, we get tension at left and equal to zero which are quite obvious results.
Hope you like it....
Mark as brainliest....
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