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The temperature of an isotropic cubical ...

The temperature of an isotropic cubical solid of length `l_(0)`, density `rho_(0)` and coefficient of linear expansion `alpha` is increased by `20^(@)C`. Then at higher temperature , to a good approximation:-

A

Length is `l_(0) (1+20alpha)`

B

Total surface area is `l_(0)^(2) (1 +40alpha)`

C

Total volume is `l_(0)^(3)(1+60alpha)`

D

Density is `(rho_(0))/(1+ 60 alpha)`

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To solve the problem step by step, we will analyze the effects of temperature change on the dimensions, surface area, volume, and density of an isotropic cubical solid. ### Step 1: Calculate the new length of the cube The linear expansion of a solid can be expressed as: \[ L = L_0 (1 + \alpha \Delta T) \] where: - \( L_0 \) is the original length, - \( \alpha \) is the coefficient of linear expansion, - \( \Delta T \) is the change in temperature. Given that the temperature is increased by \( 20^\circ C \): \[ L = L_0 (1 + \alpha \cdot 20) \] ### Step 2: Calculate the new total surface area The total surface area \( A \) of a cube is given by: \[ A = 6L^2 \] Using the new length from Step 1: \[ A = 6[L_0 (1 + \alpha \cdot 20)]^2 \] Expanding this, we have: \[ A = 6L_0^2 (1 + 20\alpha)^2 \] Using the approximation for small expansions: \[ A \approx A_0 (1 + 40\alpha) \] where \( A_0 = 6L_0^2 \). ### Step 3: Calculate the new total volume The volume \( V \) of a cube is given by: \[ V = L^3 \] Using the new length from Step 1: \[ V = [L_0 (1 + \alpha \cdot 20)]^3 \] Expanding this, we have: \[ V = L_0^3 (1 + 20\alpha)^3 \] Using the approximation for small expansions: \[ V \approx V_0 (1 + 60\alpha) \] where \( V_0 = L_0^3 \). ### Step 4: Calculate the new density Density \( \rho \) is defined as mass per unit volume: \[ \rho = \frac{m}{V} \] Since the mass \( m \) remains constant, the new density \( \rho' \) can be expressed as: \[ \rho' = \frac{\rho_0 V_0}{V} \] Substituting the volume from Step 3: \[ \rho' = \frac{\rho_0 V_0}{V_0 (1 + 60\alpha)} \] Thus: \[ \rho' = \frac{\rho_0}{1 + 60\alpha} \] ### Summary of Results 1. **New Length**: \( L = L_0 (1 + 20\alpha) \) 2. **New Total Surface Area**: \( A = 6L_0^2 (1 + 40\alpha) \) 3. **New Total Volume**: \( V = L_0^3 (1 + 60\alpha) \) 4. **New Density**: \( \rho' = \frac{\rho_0}{1 + 60\alpha} \)

To solve the problem step by step, we will analyze the effects of temperature change on the dimensions, surface area, volume, and density of an isotropic cubical solid. ### Step 1: Calculate the new length of the cube The linear expansion of a solid can be expressed as: \[ L = L_0 (1 + \alpha \Delta T) \] where: - \( L_0 \) is the original length, - \( \alpha \) is the coefficient of linear expansion, ...
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