Question #59548

a steel cable by which an elevator of mass 800kg is suspended has a diameter of 2cm.the unstretched length of the suspension cable is 10m when the elevator is on the top floor of the building.the first floor is 50m below the top floor.find the values of extension in the cable when the elevator is on the top and on the first floor.
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Expert's answer

2016-04-28T09:44:02-0400

Answer on Question #59548, Physics / Mechanics | Relativity

a steel cable by which an elevator of mass 800kg800\,\mathrm{kg} is suspended has a diameter of 2cm2\,\mathrm{cm}. The unstretched length of the suspension cable is 10m10\,\mathrm{m} when the elevator is on the top floor of the building. The first floor is 50m50\,\mathrm{m} below the top floor. Find the values of extension in the cable when the elevator is on the top and on the first floor.

Find: Δl?ε?\Delta l - ?\varepsilon - ?

Given:

- l=60ml = 60\,\mathrm{m}

- m=800kgm = 800\,\mathrm{kg}

- d=2×102md = 2 \times 10^{-2}\,\mathrm{m}

- E=210×109N/m2E = 210 \times 10^{9}\,\mathrm{N/m^2}

- g=9,8N/kgg = 9,8\,\mathrm{N/kg}

Solution:

Hooke's Law: σ=Eε(1)\sigma = E\varepsilon (1),

where σ\sigma – mechanical stress,

EE – Young's modulus,

ε\varepsilon – relative elongation.

Mechanical stress: σ=FelastS(2)\sigma = \frac{F_{\text{elast}}}{S} (2),

where FelastF_{\text{elast}} – elastic force,

SS – sectional area of the steel cable.

Elastic force numerically equal the weight of elevator:


Felast=mgF_{\text{elast}} = mg


Sectional area of the steel cable:


S=πd24S = \frac{\pi d^2}{4}


(3) and (4) in (2):


σ=4mgπd2\sigma = \frac{4\,mg}{\pi d^2}


Relative elongation: ε=Δll0(6)\varepsilon = \frac{\Delta l}{l_0} (6),

where Δl\Delta l – absolute elongation,

l0l_0 – initial length of cable.

Absolute elongation:


Δl=ll0,\Delta l = l - l_0 ,


where ll – the final length of cable

(7) in (6): ε=ll0l0\varepsilon = \frac{l - l_0}{l_0} (8)

(8) in (1): σ=E×ll0l0\sigma = E \times \frac{l - l_0}{l_0} (9)

Of (5) and (9) 4mgπd2=E×ll0l0\Rightarrow \frac{4\mathrm{mg}}{\pi d^2} = E \times \frac{l - l_0}{l_0} (10)

Of (10) 4mgl0=Eπd2(ll0)\Rightarrow 4\mathrm{mgl}_0 = \mathrm{E}\pi \mathrm{d}^2 (l - l_0) (11)

Of (11) l0(4mg+Eπd2)=Eπd2l\Rightarrow l_0(4\mathrm{mg} + \mathrm{E}\pi \mathrm{d}^2) = \mathrm{E}\pi \mathrm{d}^2 l (12)

Of (12) l0=Eπd2l(4mg+Eπd2)\Rightarrow l_0 = \frac{E\pi d^2 l}{(4mg + E\pi d^2)} (13)

Of (13) l0=59,9929m\Rightarrow l_0 = 59,9929\mathrm{m} (14)

(14) in (7): Δl=0,0071m\Delta l = 0,0071\mathrm{m} (15)

(14) and (15) in (6): ε=0,02%\varepsilon = 0,02\%

**Answer:**

Δ=7,1 mm\Delta = 7,1 \mathrm{~mm}

ε=0,02%\varepsilon = 0,02\%

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