Physics, asked by Anonymous, 7 months ago

A wire of length 2L and r is stretched between A and B without the application of any tension. If Y is the Young's modulus of the wire and it is stretched like ACB (d<<L) ,
then what will be the tension of the wire ?

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Answered by AdorableMe
56

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Correct question :-

A wire of length 2L and radius 'r' is stretched between A and B without the application of any tension. If Y is the Young's modulus of the wire and it is stretched like ACB (d<<L),  then what will be the tension of the wire ?

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Solution :-

The length of the wire is 2L.

When the wire is stretched, then the change in length can be calculated as :

\displaystyle{\frac{\delta l}{l}=\frac{l_f-l_i}{l_i}  }

\displaystyle{AC = \sqrt{l^2+d^2} }\\\\\text{(By using Pythagoras Theorem.)}

\text{The total length becomes }2\sqrt{l^2+d^2}.

As the length of BC is equal to the length of AC, and the values are added.(AB =AC+BC)

◘ Let the initial length (l_i) be 2L, and the final length (l_f) be 2\sqrt{l^2+d^2}.

\displaystyle{\frac{\delta l}{l}=\frac{2\sqrt{l^2+d^2} }{2l}} \\\\\displaystyle{\implies \frac{\delta l}{l} =\frac{l\sqrt{l+\frac{d^2}{l^2}-l } }{l} }\\\\\displaystyle{\implies \frac{\delta l}{l}=\sqrt{l+\frac{d^2}{l^2} }-l  }\\\\\displaystyle{\implies \frac{\delta l}{l}=(l+\frac{d^2}{l^2}^\frac{1}{2}  ) -1}\\\\\displaystyle{\implies \frac{\delta l}{l}=1+\frac{1}{2}*\frac{d^2}{l^2}-1   }\\\\\displaystyle{\implies \frac{\delta l}{l}=\frac{d^2}{2l^2}  }

Now, we have,

\displaystyle{y=\frac{Fl}{A \delta l} }\\\\\displaystyle{\implies F=yA\frac{\delta l}{l} }

Area of the wire = πr²

\huge\boxed{\displaystyle{\implies F=y*\pi r^2*\frac{d^2}{2l^2} }}

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*F is the tension required.

Thank you☺.

Answered by Anonymous
113

Correct question:

A wire of length 2l, and radius r is stretched between A and B without the application of any tension. If Y is the Young's modulus of the wire and it is stretched like ACB, then what will be the tension in the wire?

Theory :

Young modulus of elasticity (Y):

It is defined as the ratio of normal stress to the longitudinal strain within elastic limit.

Y = stress/strain

Solution :

Given : L = 2l

radius =r

Mean length =d

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 \sf \triangle l = (ac + bc) - 2l

Now apply Pythagoras theorem in ∆AOC

and in ∆BOC

We get AC =BC = √l²+d²

 \sf  \implies  \triangle \: l = 2 \sqrt{l {}^{2}  + d {}^{2} }  - 2l

\sf\:Stress=\dfrac{Force}{Area}

 \sf strain =  \dfrac{ \triangle l}{l}

 \sf =  \frac{  \cancel{2} (\sqrt{l {}^{2}  + d {}^{2} }  - l) }{ \cancel{2}l}

 \sf Y =  \dfrac{T}{\pi r {}^{2} }  \times  \dfrac{l}{ \sqrt{l {}^{2} + d {}^{2}  } }

 \sf T=  \dfrac{Y\pi r {}^{2}( \sqrt{l {}^{2} + d {}^{2}  }   - l)}{l}

How ,use binomial expansion

 \sf \sqrt{l {}^{2}  +d {}^{2}  }= l(1 +  \dfrac{d {}^{2} }{2l {}^{2} } )

\sf\:\sqrt{1+x}=(1+\dfrac{x}{2})

  \bf \implies T=  Y\pi r {}^{2} l(\dfrac{d {}^{2} }{2l {}^{2} } )

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