To determine the pressure difference between the inside and outside of a soap bubble, we use the concept of surface tension and the geometrical properties of the bubble.
When a bubble forms, it consists of a thin film of liquid. The bubble has two surfaces in contact with air: one on the inside and one on the outside.
The excess pressure inside a bubble is due to the surface tension acting on these two surfaces. For a soap bubble, this pressure difference can be expressed using the formula for excess pressure due to surface tension:
\(\Delta P = \frac{4S}{R}\)
The formula \(\Delta P = \frac{4S}{R}\) arises because a soap bubble has two surfaces (inside and outside). Normally, for a single surface, the formula is \(\Delta P = \frac{2S}{R}\), but since a soap bubble has two surfaces, the surface tension formula must account for both, doubling the typical expression.\
Now, let's analyze the options given:
Therefore, the correct answer is: \(\frac{4S}{R}\).
For a soap bubble, there are two liquid-air surfaces, so the excess pressure \( \Delta P \) inside the bubble is given by:
\[\Delta P = 2 \left( \frac{2S}{R} \right) = \frac{4S}{R}\]
The heat generated in 1 minute between points A and B in the given circuit, when a battery of 9 V with internal resistance of 1 \(\Omega\) is connected across these points is ______ J. 
The given circuit works as: 
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}