To solve this problem, we need to use the concepts of pressure difference and surface tension. The pressure difference caused by surface tension for an air bubble is given by the formula:
\(P_{\text{inside}} - P_{\text{outside}} = \frac{4T}{r}\)
Here, \(T\) is the surface tension of the liquid, and \(r\) is the radius of the air bubble.
Given that the pressure inside the bubble is 2100 N/m\(^2\) greater than the atmospheric pressure, we can write:
\(P_{\text{inside}} - P_{\text{outside}} = 2100 \, \text{N/m}^2\)
Also, given that the radius \(r = 0.1 \, \text{cm} = 0.001 \, \text{m}\) (converted to meters), we can substitute these values into the equation:
\(2100 = \frac{4T}{0.001}\)
Simplifying for \(T\) gives:
\(T = \frac{2100 \times 0.001}{4} = \frac{2.1}{4} = 0.525 \times 0.1 = 0.05 \, \text{N/m}\)
Therefore, the surface tension of the liquid is \(0.05 \, \text{N/m}\).
The correct answer is 0.05.
Given:
The pressure at a depth \( h \) below the surface is given by the formula: \[ P_{\text{liquid}} = \rho g h. \] Substituting the known values: \[ P_{\text{liquid}} = 1000 \times 10 \times 0.2 = 2000 \, \text{N/m}^2. \]
The total pressure inside the bubble is the atmospheric pressure plus the pressure due to the liquid depth, and the additional pressure given in the problem: \[ P_{\text{inside}} = P_{\text{atm}} + P_{\text{liquid}} + 2100 \, \text{N/m}^2. \] Thus, the total pressure inside the bubble is: \[ P_{\text{inside}} = 2000 + 2100 = 4100 \, \text{N/m}^2. \]
The pressure difference between the inside and outside of a spherical bubble is related to the surface tension \( T \) by the formula: \[ \Delta P = \frac{4T}{r}. \] Where \( r \) is the radius of the bubble. Rearranging for the surface tension \( T \): \[ T = \frac{\Delta P \times r}{4}. \] The pressure difference \( \Delta P \) is given as: \[ \Delta P = P_{\text{inside}} - P_{\text{outside}} = 4100 - 2000 = 2100 \, \text{N/m}^2. \] Substituting the known values: \[ T = \frac{2100 \times 0.001}{4} = 0.525 \, \text{N/m}. \]
The surface tension of the liquid is \( \boxed{0.05} \, \text{N/m} \).
Two liquids A and B have $\theta_{\mathrm{A}}$ and $\theta_{\mathrm{B}}$ as contact angles in a capillary tube. If $K=\cos \theta_{\mathrm{A}} / \cos \theta_{\mathrm{B}}$, then identify the correct statement:
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Two blocks of masses \( m \) and \( M \), \( (M > m) \), are placed on a frictionless table as shown in figure. A massless spring with spring constant \( k \) is attached with the lower block. If the system is slightly displaced and released then \( \mu = \) coefficient of friction between the two blocks.
(A) The time period of small oscillation of the two blocks is \( T = 2\pi \sqrt{\dfrac{(m + M)}{k}} \)
(B) The acceleration of the blocks is \( a = \dfrac{kx}{M + m} \)
(\( x = \) displacement of the blocks from the mean position)
(C) The magnitude of the frictional force on the upper block is \( \dfrac{m\mu |x|}{M + m} \)
(D) The maximum amplitude of the upper block, if it does not slip, is \( \dfrac{\mu (M + m) g}{k} \)
(E) Maximum frictional force can be \( \mu (M + m) g \)
Choose the correct answer from the options given below:
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: