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A certain number of spherical drops of a...

A certain number of spherical drops of a liquid of radius `r` coalesce to form a single drop of radius `R` and volume `V`. If `T` is the surface tension of the liquid, then

A

energy`=4VT((1)/(r )-(1)/(R ))` is released

B

energy`=3VT((1)/(r )-(1)/(R ))` is absorbed

C

energy`=3VT((1)/(r )-(1)/(R ))` is released

D

energy is neither released nor absorbed

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The correct Answer is:
To solve the problem of energy released or absorbed when a certain number of spherical drops of a liquid coalesce to form a single larger drop, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Initial and Final States**: - We have `n` small drops, each with a radius `r`. - These drops coalesce to form one larger drop with radius `R`. 2. **Calculate the Volume**: - The volume of one small drop is given by: \[ V_{\text{small}} = \frac{4}{3} \pi r^3 \] - Therefore, the total volume of `n` small drops is: \[ V_{\text{total}} = n \cdot V_{\text{small}} = n \cdot \frac{4}{3} \pi r^3 \] - The volume of the larger drop is: \[ V_{\text{large}} = \frac{4}{3} \pi R^3 \] - Since volume is conserved, we set these equal: \[ n \cdot \frac{4}{3} \pi r^3 = \frac{4}{3} \pi R^3 \] - Simplifying gives: \[ n r^3 = R^3 \quad \Rightarrow \quad n = \frac{R^3}{r^3} \] 3. **Calculate Surface Energy**: - The surface energy of a drop is given by: \[ \text{Surface Energy} = \text{Surface Area} \times \text{Surface Tension} \] - For one small drop: \[ \text{Surface Energy}_{\text{small}} = 4 \pi r^2 T \] - For `n` small drops: \[ \text{Total Surface Energy}_{\text{small}} = n \cdot 4 \pi r^2 T = \frac{R^3}{r^3} \cdot 4 \pi r^2 T = 4 \pi R^3 \frac{T}{r} \] - For the larger drop: \[ \text{Surface Energy}_{\text{large}} = 4 \pi R^2 T \] 4. **Calculate Change in Surface Energy**: - The change in surface energy (ΔE) when the drops coalesce is: \[ \Delta E = \text{Surface Energy}_{\text{large}} - \text{Total Surface Energy}_{\text{small}} \] - Substituting the expressions we found: \[ \Delta E = 4 \pi R^2 T - 4 \pi R^3 \frac{T}{r} \] - Factoring out \(4 \pi T\): \[ \Delta E = 4 \pi T \left( R^2 - \frac{R^3}{r} \right) \] 5. **Final Expression**: - This can be simplified to: \[ \Delta E = 4 \pi T \left( R^2 - R^3 \frac{1}{r} \right) \] - This expression represents the energy absorbed or released during the coalescence process.

To solve the problem of energy released or absorbed when a certain number of spherical drops of a liquid coalesce to form a single larger drop, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Initial and Final States**: - We have `n` small drops, each with a radius `r`. - These drops coalesce to form one larger drop with radius `R`. ...
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