
Given that \( T \) is constant: \[ PV = \text{constant} \]
From this, we get the relation between pressure and volume: \[ P \propto \frac{1}{V} \]
If the volume changes by a factor of \( \frac{100}{101} \), the pressure changes by a factor of \( \frac{101}{100} \). Thus, the pressure becomes: \[ P_f = 1.01 \times P_0 \]
The equation for the pressure difference is: \[ P_0 - \frac{2T}{R} = 1.01 P_0 - \rho g h \]
Rearranging this to solve for \( \rho g h \): \[ \rho g h = 0.01 P_0 + \frac{2T}{R} \]
Now, substituting the given values: \[ (10^3)(10)h = (0.01)(10^5) + \frac{2 \times 0.075}{0.1 \times 10^{-3}} \]
Solving for \( h \): \[ h = \frac{2500}{10^4} \, \text{m} = 25 \, \text{cm} \]
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
The science of the mechanical properties of fluids is called Hydrostatics. A fluid is a substance that relents to the slightest pressure. Fluids are categorized into two classes famed by the names of liquids, and elastic fluids or gases, which later comprehend the air of the atmosphere and all the different kinds of air with which chemistry makes us acquainted.
A streamline is a curve the tangent to which at any point provides the direction of the fluid velocity at that point. It is comparable to a line of force in an electric or magnetic field. In steady flow, the pattern of the streamline is motionless or static with time, and therefore, a streamline provides the actual path of a fluid particle.
A tubular region of fluid enclosed by a boundary comprises streamlines is called a tube of flow. Fluid can never cross the boundaries of a tube of flow and therefore, a tube of flow acts as a pipe of the same shape.
The surface tension of a liquid is all the time a function of the solid or fluid with which the liquid is in contact. If a value for surface tension is provided in a table for oil, water, mercury, or whatever, and the contacting fluid is unspecified, it is safe to consider that the contacting fluid is air.