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A massive stone pillar 20 m high and of ...

A massive stone pillar `20 m` high and of uniform cross section rests on a rigid base and supports a vertical load of `5.0 xx 10^(5)N` at its upper end. If the compressive stress in the pillar is not exceed `1.6 xx10^(6)N//m^2`, what is the minimum cross-sectional area of the pillar? (Density of the stone `=2.5xx10^(3) kg//m^(3)` take `g= 10 N//kg)`

A

`0.15m^(2)`

B

`0.25m^(2)`

C

`0.35m^(2)`

D

`0.45m^(2)`

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To solve the problem step by step, we need to determine the minimum cross-sectional area of the stone pillar that can support the given load without exceeding the specified compressive stress. ### Step 1: Understand the Given Data - Height of the pillar, \( h = 20 \, m \) - Load on the pillar, \( F = 5.0 \times 10^5 \, N \) - Maximum compressive stress, \( \sigma_{max} = 1.6 \times 10^6 \, N/m^2 \) - Density of the stone, \( \rho = 2.5 \times 10^3 \, kg/m^3 \) - Acceleration due to gravity, \( g = 10 \, N/kg \) ### Step 2: Calculate the Weight of the Pillar The weight \( W \) of the pillar can be calculated using the formula: \[ W = m \cdot g \] Where \( m \) is the mass of the pillar. The mass can be calculated from the density and volume: \[ m = \rho \cdot V \] The volume \( V \) of the pillar can be expressed as: \[ V = A \cdot h \] Where \( A \) is the cross-sectional area. Thus, we can write: \[ m = \rho \cdot (A \cdot h) \] Substituting this into the weight formula: \[ W = \rho \cdot (A \cdot h) \cdot g \] ### Step 3: Calculate the Total Force Acting on the Pillar The total force \( F_{total} \) acting on the pillar is the sum of the applied load and the weight of the pillar: \[ F_{total} = F + W = F + \rho \cdot (A \cdot h) \cdot g \] ### Step 4: Write the Stress Formula The stress \( \sigma \) in the pillar is given by: \[ \sigma = \frac{F_{total}}{A} \] Substituting for \( F_{total} \): \[ \sigma = \frac{F + \rho \cdot (A \cdot h) \cdot g}{A} \] ### Step 5: Set Up the Equation We know that the stress must not exceed the maximum compressive stress: \[ 1.6 \times 10^6 = \frac{5.0 \times 10^5 + \rho \cdot (A \cdot h) \cdot g}{A} \] Substituting \( \rho \), \( h \), and \( g \): \[ 1.6 \times 10^6 = \frac{5.0 \times 10^5 + (2.5 \times 10^3) \cdot (A \cdot 20) \cdot 10}{A} \] ### Step 6: Simplify the Equation This simplifies to: \[ 1.6 \times 10^6 = \frac{5.0 \times 10^5 + 5.0 \times 10^4 \cdot A}{A} \] Multiplying through by \( A \): \[ 1.6 \times 10^6 A = 5.0 \times 10^5 + 5.0 \times 10^4 A \] ### Step 7: Rearranging the Equation Rearranging gives: \[ 1.6 \times 10^6 A - 5.0 \times 10^4 A = 5.0 \times 10^5 \] \[ (1.6 \times 10^6 - 5.0 \times 10^4) A = 5.0 \times 10^5 \] \[ (1.55 \times 10^6) A = 5.0 \times 10^5 \] ### Step 8: Solve for Area \( A \) Now, solving for \( A \): \[ A = \frac{5.0 \times 10^5}{1.55 \times 10^6} \] Calculating this gives: \[ A \approx 0.3226 \, m^2 \] ### Step 9: Conclusion Thus, the minimum cross-sectional area of the pillar is approximately \( 0.3226 \, m^2 \).

To solve the problem step by step, we need to determine the minimum cross-sectional area of the stone pillar that can support the given load without exceeding the specified compressive stress. ### Step 1: Understand the Given Data - Height of the pillar, \( h = 20 \, m \) - Load on the pillar, \( F = 5.0 \times 10^5 \, N \) - Maximum compressive stress, \( \sigma_{max} = 1.6 \times 10^6 \, N/m^2 \) - Density of the stone, \( \rho = 2.5 \times 10^3 \, kg/m^3 \) - Acceleration due to gravity, \( g = 10 \, N/kg \) ...
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