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Two soap bubble are combined isothermall...

Two soap bubble are combined isothermally to form a big bubble of radius R. If `DeltaV` is change in volume, `DeltaS` is change in surface area and `P_(0)` is atmospheric pressure then show that `3P_(0)(DeltaV)+4T(DeltaS)=0`

A

`4pV+3SA=0`

B

`3pV-4SA=0`

C

`4pV-3SA=0`

D

`3pV+4SA=0`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to analyze the situation of two soap bubbles combining into a larger bubble and derive the relationship between the change in volume (ΔV) and the change in surface area (ΔS) under isothermal conditions. ### Step-by-Step Solution: 1. **Understand the Initial Conditions**: - Let the radii of the two soap bubbles be \( r_A \) and \( r_B \). - The pressure inside a soap bubble is given by \( P = P_0 + \frac{4T}{r} \), where \( P_0 \) is the atmospheric pressure and \( T \) is the surface tension. 2. **Calculate the Initial Pressures**: - For bubble A: \[ P_A = P_0 + \frac{4T}{r_A} \] - For bubble B: \[ P_B = P_0 + \frac{4T}{r_B} \] 3. **Calculate the Pressure of the Combined Bubble**: - After combining, let the radius of the new bubble be \( R \): \[ P = P_0 + \frac{4T}{R} \] 4. **Apply the Isothermal Condition**: - The isothermal condition implies that the total pressure times the total volume before combining equals the total pressure times the total volume after combining: \[ P_A V_A + P_B V_B = P V \] - The volumes of the bubbles are given by: \[ V_A = \frac{4}{3} \pi r_A^3, \quad V_B = \frac{4}{3} \pi r_B^3, \quad V = \frac{4}{3} \pi R^3 \] 5. **Substituting the Volumes**: - Substitute the expressions for pressure and volume into the equation: \[ \left(P_0 + \frac{4T}{r_A}\right) \left(\frac{4}{3} \pi r_A^3\right) + \left(P_0 + \frac{4T}{r_B}\right) \left(\frac{4}{3} \pi r_B^3\right) = \left(P_0 + \frac{4T}{R}\right) \left(\frac{4}{3} \pi R^3\right) \] 6. **Simplifying the Equation**: - Cancel \( \frac{4}{3} \pi \) from both sides: \[ \left(P_0 + \frac{4T}{r_A}\right) r_A^3 + \left(P_0 + \frac{4T}{r_B}\right) r_B^3 = \left(P_0 + \frac{4T}{R}\right) R^3 \] - Rearranging gives: \[ P_0 (r_A^3 + r_B^3 - R^3) + 4T \left(\frac{r_A^3}{r_A} + \frac{r_B^3}{r_B} - \frac{R^3}{R}\right) = 0 \] 7. **Expressing Change in Volume and Surface Area**: - The change in volume \( \Delta V \) is: \[ \Delta V = \frac{4}{3} \pi (r_A^3 + r_B^3 - R^3) \] - The change in surface area \( \Delta S \) is: \[ \Delta S = 4\pi R^2 - 4\pi r_A^2 - 4\pi r_B^2 \] 8. **Substituting ΔV and ΔS**: - Substitute \( \Delta V \) and \( \Delta S \) into the rearranged equation: \[ P_0 \Delta V + 4T \left(-\frac{\Delta S}{4\pi}\right) = 0 \] - This leads to: \[ 3P_0 \Delta V + 4T \Delta S = 0 \] ### Final Result: Thus, we have shown that: \[ 3P_0 \Delta V + 4T \Delta S = 0 \]
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