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A steel cable with a radius 2 cm support...

A steel cable with a radius 2 cm supports a chairlift at a ski area. If the maximum stress is not to exceed `10^8 N m^(-2)`, the maximam load the cable can support

A

`4pi xx 10^(5)N`

B

`4pi xx 10^(4) N`

C

`2pi xx 10^(5) N`

D

`2pi xx 10^(4)`

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The correct Answer is:
To solve the problem of determining the maximum load that a steel cable can support without exceeding a maximum stress of \(10^8 \, \text{N/m}^2\), we can follow these steps: ### Step 1: Understand the relationship between stress, force, and area Stress (\(\sigma\)) is defined as the force (F) applied per unit area (A): \[ \sigma = \frac{F}{A} \] ### Step 2: Rearrange the formula to find the force From the formula, we can rearrange it to find the force: \[ F = \sigma \cdot A \] ### Step 3: Calculate the area of the cable The area (A) of a circular cross-section can be calculated using the formula: \[ A = \pi r^2 \] where \(r\) is the radius of the cable. Given that the radius is 2 cm, we need to convert it to meters: \[ r = 2 \, \text{cm} = 0.02 \, \text{m} \] Now, we can calculate the area: \[ A = \pi (0.02)^2 = \pi (0.0004) = 0.0004\pi \, \text{m}^2 \] ### Step 4: Substitute the values into the force equation Now we can substitute the maximum stress and the area into the force equation: \[ F = (10^8 \, \text{N/m}^2) \cdot (0.0004\pi \, \text{m}^2) \] \[ F = 10^8 \cdot 0.0004\pi = 4 \times 10^4 \pi \, \text{N} \] ### Step 5: Calculate the numerical value Using the approximate value of \(\pi \approx 3.14\): \[ F \approx 4 \times 10^4 \times 3.14 \approx 125600 \, \text{N} \] ### Step 6: Final result Thus, the maximum load the cable can support is approximately: \[ F \approx 125600 \, \text{N} \]

To solve the problem of determining the maximum load that a steel cable can support without exceeding a maximum stress of \(10^8 \, \text{N/m}^2\), we can follow these steps: ### Step 1: Understand the relationship between stress, force, and area Stress (\(\sigma\)) is defined as the force (F) applied per unit area (A): \[ \sigma = \frac{F}{A} \] ...
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When a tensile or compressive load 'P' is applied to rod or cable, its length changes. The change length x which, for an elastic material is proportional to the force Hook' law). P alpha x or P = kx The above equation is similar to the equation of spring. For a rod of length L , area A and young modulue Y . the extension x can be expressed as. x = (PL)/(AY) or P = (AY)/(x) , hence K = (AY)/(L) Thus rod or cables attached to lift can be treated as springs. The energy stored in rod is called strain energy & equal to (1)/(2)Px . The loads placed or dropped on the floor of lift cause stresses in the cable and can be evaluted by spring analogy. If the cable of lift cause stresses and load is placed dropped, then maximum extension in cable can be calculated by energy conservation. In above problem if mass of 10 kg falls on the massless collar attached to rod from the height of 99cm then maximum extension in the rod is equal (rod of length 4m, area 4cm^(2) and young modules 2 xx 10^(10)N//m^(2) g = 10m//sec^(2) )-

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When a tensile or compressive load 'P' is applied to rod or cable, its length changes. The change length x which, for an elastic material is proportional to the force Hook' law). P alpha x or P = kx The above equation is similar to the equation of spring. For a rod of length L , area A and young modulue Y . the extension x can be expressed as. x = (PL)/(AY) or P = (AY)/(x) , hence K = (AY)/(L) Thus rod or cables attached to lift can be treated as springs. The energy stored in rod is called stra energy & equal to (1)/(2)Px . The loads placed or dropped on the floor of lift cause stresses in the cable and can be evaluted by spring analogy. If the cable of lift cause stresses and load is placed dropped, then maximum extension in cable can be calculated by enerfy conservation. It two rods of same length (4m) and cross section areas 2 cm^(2) and 4 cm^(2) with same young modulus 2 xx 10^(10)N//m^(2) are attached one after the other with mass 600 kg then angular frequency is-

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