A steel wire of mass µ per unit length with a circular cross section has a radius of 0.1 cm. The wire is of length 10 m when measured lying horizontal, and hangs from a hook on the wall. A mass of 25 kg is hung from the free end of the wire. Assuming the wire to be uniform and lateral strains << longitudinal strains, find the extension in the length of the wire. The density of steel is 7860 kg m–3 (Young’s modules Y=2×1011 Nm–2). (b) If the yield strength of steel is 2.5×108 Nm–2, what is the maximum weight that can be hung at the lower end of the wire?

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    Answered by

    Payal Gupta | Contributor-Level 10

    4 months ago

    This is a long answer type question as classified in NCERT Exemplar

    When a small element of length dx is considered at x from the load x=0

    (a) letT(x) and T(x+dx) are tensions on the two cross sections a distance dx apart then

    T(x+dx)+T(x)=dmg= μ dxg

    dT= μ gx+C

    at x=0 T(0)=mg

    C=mg

    T(x)= μ gx+Mg

    Let length dx at x increases by dr then

    Young’s modulus Y= stress/strain

    T x A d r d x = Y

    d r d x = T x Y A

    r= 1 Y A 0 L ( μ g x + M g ) d x

    = 1 Y A μ g x 2 2 + M g x 0L

    r= 1 2 × 10 11 × π × 10 - 6 π × 786 × 10 - 3 × 10 × 10 2 + 25 × 10 × 10

     

    so r = 4 × 10 - 3 m

    (b) tension will be maximum at x=L

    T= μ g L +Mg=(m+M)g

    The force = (yield strength) area= 250 × π N

    (m+M)g= 250 π

    Mg 250 π

    M= 25 π 75 k g

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Vishal Baghel

If μ  is Poisson’s ratio,

Y = 3K (1 - 2 μ )      ……… (1)

and Y = 2 n ( 1 + μ )  ……… (2)

With the help of equations (1) and (2), we can write

  3 Y = 1 η + 1 3 k K = η Y 9 η 3 Y

V
Vishal Baghel

dm = (m/L)dx
∴ T = (mω²/2L) (L² - x²)
∴ ΔL = ∫? (mω²/2Lπr²Y) (L² - x²)dx
= ΔL = mω²L²/3πr²Y

V
Vishal Baghel

Initially S? L = 2m
S? L = √2² + (3/2)²
S? L = 5/2 = 2.5 m
? x = S? L - S? L = 0.5 m
So since λ = 1 m. ∴? x = λ/2
So white listener moves away from S? Then? x (= S? L − S? L) increases and hence, at? x = λ first maxima will appear.? x = λ = S? L − S? L.
1 = d - 2 ⇒ d = 3 m.

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Vishal Baghel

Loss in elastic potential energy = Gain in KE
½ (YA/L)x² = ½mv²
0.5 × (0.5×10? × 10? / 0.1) × (0.04)² = 20×10? ³ v²
0.5 × (5×10²) × 1.6×10? ³ = 20×10? ³ v²
0.4 = 20×10? ³ v²
v² = 20 => v = √20 ≈ 4.47 m/s
(Re-checking calculations)
0.5 * ( (0.5e9 * 1e-6) / 0.1) * (0.04)^2 = 0.5 * (5e2) * 1.6e-3 = 4.
0.5 * 20e-3 * v^2 = 10e-3 v^2
4 = 10e-3 v^2
v^2 = 400 => v = 20 m/s

V
Vishal Baghel

As we know that

Y = F L A ? L          

? L = 0 . 0 4 m = F L A Y . . . . . . . . . . . . . . . ( i )           

If length and diameter both are doubled

? L ' = F . 2 L 4 A . Y = F L 2 Y = 0 . 0 2 m = 2 c m       

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