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.If 1000 droplets of water of surface te...

.If `1000` droplets of water of surface tension `0.07N/m`,having same radius `1mm` each,combine to from a single drop.In the process the released surface energy is : (Take `pi=(22)/(7)`

A

`8.8 xx 10^-5 J`

B

`7.92 xx 10^-4 J`

C

`7.92 xx10^-6 J`

D

`9.68 xx 10^-4 J`

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To solve the problem of calculating the released surface energy when 1000 droplets of water combine into a single drop, we will follow these steps: ### Step 1: Understand the Given Data - Number of droplets, \( n = 1000 \) - Surface tension, \( \sigma = 0.07 \, \text{N/m} \) - Radius of each droplet, \( r = 1 \, \text{mm} = 1 \times 10^{-3} \, \text{m} \) ### Step 2: Calculate the Initial Volume of the 1000 Droplets The volume \( V \) of a single droplet is given by the formula for the volume of a sphere: \[ V = \frac{4}{3} \pi r^3 \] For 1000 droplets, the total initial volume \( V_i \) is: \[ V_i = n \cdot V = 1000 \cdot \frac{4}{3} \pi r^3 \] ### Step 3: Calculate the Final Volume of the Single Large Drop Let the radius of the final large drop be \( R \). The volume of the single large drop \( V_f \) is: \[ V_f = \frac{4}{3} \pi R^3 \] By the principle of volume conservation, we have: \[ V_i = V_f \] Thus, \[ 1000 \cdot \frac{4}{3} \pi r^3 = \frac{4}{3} \pi R^3 \] Cancelling \( \frac{4}{3} \pi \) from both sides gives: \[ 1000 \cdot r^3 = R^3 \] ### Step 4: Solve for the Radius of the Final Drop Substituting \( r = 1 \times 10^{-3} \, \text{m} \): \[ R^3 = 1000 \cdot (1 \times 10^{-3})^3 = 1000 \cdot 10^{-9} = 10^{-6} \] Taking the cube root: \[ R = (10^{-6})^{1/3} = 10^{-2} \, \text{m} = 10 \, \text{mm} \] ### Step 5: Calculate the Surface Energy of the Initial and Final Drops The surface energy \( U \) is given by: \[ U = \sigma \cdot A \] where \( A \) is the surface area. The surface area \( A \) of a sphere is given by: \[ A = 4 \pi r^2 \] #### Initial Surface Energy \( U_1 \) For the 1000 droplets: \[ U_1 = n \cdot \sigma \cdot (4 \pi r^2) = 1000 \cdot 0.07 \cdot (4 \pi (1 \times 10^{-3})^2) \] Calculating \( U_1 \): \[ U_1 = 1000 \cdot 0.07 \cdot (4 \pi \cdot 10^{-6}) = 0.07 \cdot 4 \cdot \frac{22}{7} \cdot 10^{-3} \] \[ U_1 = 0.07 \cdot 4 \cdot 3.14 \cdot 10^{-3} \approx 0.07 \cdot 12.56 \cdot 10^{-3} \approx 0.000878 \, \text{J} \] #### Final Surface Energy \( U_2 \) For the single large drop: \[ U_2 = \sigma \cdot (4 \pi R^2) = 0.07 \cdot (4 \pi (10 \times 10^{-3})^2) \] Calculating \( U_2 \): \[ U_2 = 0.07 \cdot (4 \pi \cdot 10^{-4}) = 0.07 \cdot 4 \cdot \frac{22}{7} \cdot 10^{-4} \] \[ U_2 = 0.07 \cdot 12.56 \cdot 10^{-4} \approx 0.000878 \cdot 10^{-1} \approx 0.0000878 \, \text{J} \] ### Step 6: Calculate the Released Surface Energy The released surface energy \( U_{\text{released}} \) is given by: \[ U_{\text{released}} = U_1 - U_2 \] Calculating: \[ U_{\text{released}} = 0.000878 - 0.0000878 \approx 0.0007902 \, \text{J} \] ### Final Answer The released surface energy when the droplets combine to form a single drop is approximately: \[ \boxed{0.0007902 \, \text{J}} \]
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