A twisted steel clothesline wire of length l has cross-sectional area A and modulus of elasticity in tension E . The wire is stretched horizontally between two fixed points A and B , but without appreciable initial tension. A load P is then suspended from the mid-point C of the line. The vertical deflection of the point C can be expressed as δ = m l n A E P where m and n are co-prime. Find m + n .
DETAILS AND ASSUMPTIONS:
∙ The deflection is small compared to the length l of the clothesline.
∙ This problem has been taken directly from a book.
∙ A clear solution would be greatly appreciated(as I can't solve it).
∙ This is my first problem.
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Thanks for the solution.
For equilibrium,
2
T
sin
θ
=
P
Using given condition, sin θ ≈ θ ≈ tan θ
2 T tan θ = P
2 T 2 l x = P
l 4 T x = P
Now, let us find the extension in the wire.
Δ l = 2 ( 2 l ) 2 + x 2 − l
Using Binomial expansion and simplifying the result,
Δ l = l 2 x 2
Using the definition of Young's Modulus,
E = Strain Stress = l Δ l A T
E = 8 A x 3 P l 3
Thus,
x = 2 l ( A E P ) 3 1
Hence,
m + n = 5
Ok. So finally a(two) good solution(s) have come up. Great!!!
Congrats for META in IIT-B. Enjoy.... :)
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Thank You. What did you get?
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Hey I am currently pursuing B.E. in ME from JU.
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Solution
F i r s t n o t e t h a t A C = C B = l / 2 w h e r e l i s t h e t o t a l l e n g t h o f t h e w i r e . B y o b s e r v i n g t h e F B D o n t h e l o a d a n d w r i t i n g e q u a t i o n f o r e q u i l i b r i u m w e g e t : 2 F s i n ( θ ) = P ( i ) N o w A D = l s e c ( θ ) / 2 ⇒ E l o n g a t i o n = Δ l = A D − A C = l / 2 ( s e c ( θ ) − 1 ) ( i i ) N o w w r i t i n g t h e e q u a t i o n S t r a i n S t r e s s = M o d u l u s o f e l a s t i c i t y w e g e t Δ l / ( l / 2 ) F / A = E h e n c e F = l 2 Δ l E A . P u t t i n g t h e v a l u e o f Δ l w e g e t F = E A ( s e c ( θ ) − 1 ) = E A ( c o s ( θ ) 1 − c o s ( θ ) ) = c o s ( θ ) 2 E A s i n 2 ( θ / 2 ) ( i i i ) H e r e c o m e s t h e t r i c k s i n c e θ ≈ 0 w e c a n w r i t e s i n ( θ ) ≈ θ a n d c o s ( θ ) ≈ 1 a n d t a n ( θ ) ≈ θ s o e q u a t i o n ( i i i ) b e c o m e s F = E A θ 2 / 2 p u t t i n g v a l u e o f F i n e q . ( 1 ) w e g e t P = ( 2 θ ) ( E A θ 2 / 2 ) = E A θ 3 S o l v i n g θ = 3 E A P ( i v ) N o w o u r v e r t i c a l e l o n g a t i o n δ = l t a n ( θ ) / 2 ≈ l θ / 2 U s i n g e q u a t i o n ( i v ) w e g e t δ = 2 l 3 E A P S o m = 2 , n = 3 h e n c e m + n = 5