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Question: Two spherical soap bubbles of a radii \( {{\text{r}}_1} \) and \( {{\text{r}}_2} \) in vacuum coales...

Two spherical soap bubbles of a radii r1{{\text{r}}_1} and r2{{\text{r}}_2} in vacuum coalesce under isothermal conditions. The resulting bubble has the radius RR such that:
(A) R=r1+r2{\text{R}} = {{\text{r}}_1} + {{\text{r}}_2}
(B) R2=r12+r22{{\text{R}}^2} = {\text{r}}_1^2 + {\text{r}}_2^2
(C) R=r1+r2r2{\text{R}} = \dfrac{{{{\text{r}}_1} + {{\text{r}}_2}}}{{{{\text{r}}_2}}}
(D) None of these

Explanation

Solution

Boyle's law is a gas law which states that the pressure exerted by a gas(of a given mass, maintained at a constant temperature) is inversely proportional to the volume occupied by it. In other words, as long as the temperature and the amount of gas are kept constant, the pressure and volume of a gas are inversely proportional to each other.

Complete step by step answer:
It is given that the radius of both the soap bubbles are r1{r_1} and r2{r_2}
Under isothermal conditions, we have
P1V1=P2V2{P_1}{V_1} = {P_2}{V_2}
Also, it is given that the bubbles are in vacuum. This means that the only pressure acting will be on the bubble surface because of surface tension
So, the pressure in the first soap bubble is given by
P1=4Sr1{P_1} = \dfrac{{4S}}{{{r_1}}}
And the volume of the first soap bubble is given by
V1=43πr13{V_1} = \dfrac{4}{3}\pi {r_1}^3
Therefore
P1V1=4Sr1×43πr13{P_1}{V_1} = \dfrac{{4S}}{{{r_1}}} \times \dfrac{4}{3}\pi {r_1}^3
Similarly, for the second soap bubble
P2V2=4Sr2×43πr23{P_2}{V_2} = \dfrac{{4S}}{{{r_2}}} \times \dfrac{4}{3}\pi {r_2}^3
Under isothermal conditions, bot these bubbles merge to form third bubble of radius RR
So, the pressure of the third bubble will be
P3=4SR{P_3} = \dfrac{{4S}}{R}
Also, the volume of this bubble is given by
V3=43πR3{V_3} = \dfrac{4}{3}\pi {R^3}
So, we get
P3V3=4SR×43πR3{P_3}{V_3} = \dfrac{{4S}}{R} \times \dfrac{4}{3}\pi {R^3}
We know that
PV=nRTPV = nRT
Since both the bubbles are merging to form a bigger bubble. The temperature remains constant, the number of moles of the first bubble will add up with the number of moles of the second bubble to form the third big bubble.
So, we can write
P3V3=P1V1+P2V2{P_3}{V_3} = {P_1}{V_1} + {P_2}{V_2}
Now we will substitute the values of each of these terms in the above equation to get
4SR×43πR3=4Sr1×43πr13+4Sr2×43πr23\dfrac{{4S}}{R} \times \dfrac{4}{3}\pi {R^3} = \dfrac{{4S}}{{{r_1}}} \times \dfrac{4}{3}\pi {r_1}^3 + \dfrac{{4S}}{{{r_2}}} \times \dfrac{4}{3}\pi {r_2}^3
We can rewrite above equation as
4S(43πR2)=4S(43π)(r12+r22)4S\left( {\dfrac{4}{3}\pi {R^2}} \right) = 4S\left( {\dfrac{4}{3}\pi } \right)\left( {{r_1}^2 + {r_2}^2} \right)
Hence, upon further solving, we get
R2=r12+r22{R^2} = {r_1}^2 + {r_2}^2
The correct option is (B.)

Note:
The pressure inside the bubble must be higher than the pressure on the outside for the bubble to be stable and not collapse. The force must balance the strength of the surface tension with the pressure difference.