Analyze Statement I:
Statement I states that when the speed of liquid is zero everywhere, the pressure difference at any two points depends on the equation:
\[ P_1 - P_2 = \rho g(h_2 - h_1) \]
This is correct and is based on the hydrostatic pressure difference, which applies when the fluid is at rest or moving uniformly without velocity gradients.
Analyze Statement II Using Bernoulli’s Equation:
In a venturi tube, where the fluid is in motion, we can apply Bernoulli’s equation:
\[ P_1 + \rho gh + \frac{1}{2}\rho v_1^2 = P_2 + \rho gh + \frac{1}{2}\rho v_2^2 \]
Simplifying for the pressure difference, we get:
\[ P_1 - P_2 = \frac{1}{2}\rho (v_2^2 - v_1^2) \]
The statement given, \(2gh = v_2^2 - v_1^2\), is not a general result of Bernoulli’s equation and is incorrect as presented.
Conclusion:
Therefore, Statement I is correct (it applies to a static fluid or uniform motion with no speed variations), but Statement II is incorrect in the context of the venturi tube.
Consider the following statements:
A. Surface tension arises due to extra energy of the molecules at the interior as compared to the molecules at the surface of a liquid.
B. As the temperature of liquid rises, the coefficient of viscosity increases.
C. As the temperature of gas increases, the coefficient of viscosity increases.
D. The onset of turbulence is determined by Reynolds number.
E. In a steady flow, two streamlines never intersect.
Choose the correct answer from the options given below:
$\text{The fractional compression } \left( \frac{\Delta V}{V} \right) \text{ of water at the depth of } 2.5 \, \text{km below the sea level is } \_\_\_\_\_\_\_\_\_\_ \%. \text{ Given, the Bulk modulus of water } = 2 \times 10^9 \, \text{N m}^{-2}, \text{ density of water } = 10^3 \, \text{kg m}^{-3}, \text{ acceleration due to gravity } g = 10 \, \text{m s}^{-2}.$
Match List - I with List - II:
List - I:
(A) Electric field inside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(B) Electric field at distance \( r > 0 \) from a uniformly charged infinite plane sheet with surface charge density \( \sigma \).
(C) Electric field outside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(D) Electric field between two oppositely charged infinite plane parallel sheets with uniform surface charge density \( \sigma \).
List - II:
(I) \( \frac{\sigma}{\epsilon_0} \)
(II) \( \frac{\sigma}{2\epsilon_0} \)
(III) 0
(IV) \( \frac{\sigma}{\epsilon_0 r^2} \) Choose the correct answer from the options given below: