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A glass rod of radius \(r_{1}\) is inserted symmetrically into a vertical capillary tube of radius \(r_{2}\) such that their lower ends are at the same level. The arrangement is now dipped in water. The height to which water will rise into the tube will be ( \(\sigma=\) surface tension of water, \(\rho=\) density of water) (1) \(\frac{2 \sigma}{\left(r_{2}-r_{1}\right) \rho g}\) (2) \(\frac{\sigma}{\left(r_{2}-r_{1}\right) \rho g}\) (3) \(\frac{2 \sigma}{\left(r_{2}+r_{1}\right) \rho g}\) (4) \(\frac{2 \sigma}{\left(r_{2}^{2}+r_{1}^{2}\right) \rho g}\)

Short Answer

Expert verified
Option (1): \(\frac{2\sigma}{(r_2 - r_1)\rho g}\).

Step by step solution

01

Understanding the Setup

We have a vertical capillary tube with radius \( r_2 \) into which a glass rod with radius \( r_1 \) is symmetrically inserted. This forms a small annular gap for water to rise within, between the rod and the tube.
02

Analyzing the Capillary Action

Using the principle of capillary action, where the surface tension drives the liquid up the tube, we recognize that the effective radius of the gap is the difference in radii: \( r_2 - r_1 \). Thus, we will apply the formula for the capillary rise, considering the effective radius as \( r_2 - r_1 \).
03

Applying the Capillary Rise Formula

The height \( h \) of liquid rise due to capillarity is given by the formula \( h = \frac{2 \sigma}{r \rho g} \), where \( \sigma \) is the surface tension of the liquid, \( \rho \) is the density of the liquid, and \( g \) is the acceleration due to gravity. Here, the effective radius \( r = r_2 - r_1 \).
04

Calculation of Water Rise Height

Substituting the effective radius into the capillary rise formula, we get \( h = \frac{2 \sigma}{(r_2 - r_1) \rho g} \). This means the height to which the water will rise is dependent on the difference in the radii of the tube and the rod.
05

Selecting the Correct Option

Comparing our derived expression \( \frac{2 \sigma}{(r_2 - r_1) \rho g} \) with the given options, we find that it matches option (1). Thus, option (1) is the correct answer.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Surface Tension
Surface tension is a fascinating property of liquids that causes them to behave as though their surface is covered with an invisible stretched elastic membrane. This property is especially significant in capillary action, which is the process that allows liquids to flow in narrow spaces without external forces. In the context of capillary action, surface tension is the driving force that causes liquid to rise in a tube.
Surface tension arises due to cohesive forces, which are the attractive forces between molecules of the same substance. These forces are strongest at the surface of the liquid, as the molecules at the surface lack neighboring molecules above them. This results in the surface behaving like a stretched elastic film.
  • The magnitude of surface tension directly influences how much a liquid can rise in a capillary tube.
  • In water, these forces are particularly strong due to hydrogen bonding.
Density of Water
Density is a measure of how much mass is contained in a given volume. For water, the density is conventionally taken to be approximately 1000 kg/m³ under standard conditions. It is an important factor in hydrostatics and capillary action.
In the context of capillary rise, density affects the height to which the liquid ascends. This is because the weight of the column of liquid must be balanced by the upward force contributed by surface tension.
  • An increased density would result in a lesser height of climb, due to greater downward gravitational force.
  • Density also influences the buoyancy and stability of objects submerged or floating in water.
Hydrostatics
Hydrostatics is the branch of fluid mechanics that deals with fluids at rest. It often concerns the study of pressure in liquids and gases. In the realm of capillary action, hydrostatics helps explain the equilibrium between the gravitational force pulling the liquid down and the surface tension pulling it up. This balance determines the height to which the liquid rises.
To understand this balance, remember that the weight of the liquid is given by its volume, density, and gravitational acceleration. Against this, the surface tension creates a force, which is significant in narrow tubes.
  • Gravity acts to pull the liquid downwards, creating hydrostatic pressure.
  • Surface tension counteracts this pressure, allowing liquid to rise against gravity.
Capillary Rise Formula
The capillary rise formula is a mathematical representation used to calculate the height a liquid will rise in a capillary tube. It can be expressed as \( h = \frac{2\sigma}{r \rho g} \), where:
  • \( h \) is the height of the rise.
  • \( \sigma \) is the surface tension of the liquid.
  • \( r \) is the effective radius.
  • \( \rho \) is the liquid's density.
  • \( g \) is the acceleration due to gravity.

Understanding this formula requires breaking down each term:
  • The expression \( \frac{2\sigma}{r} \) represents how the pull of surface tension scales with the inverse of the radius.
  • The product \( \rho g \) accounts for the gravitational force acting downward on the liquid column.
The formula demonstrates that smaller radii, higher surface tension, or lower density can result in greater heights of liquid rise. In the given exercise, the effective radius \( r \) is adjusted for the annular gap, calculated as \( r_2 - r_1 \), altering the entire dynamics of the situation.

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Most popular questions from this chapter

A water drop is divided into eight equal droplets. The pressure difference between inner and outer sides of the big drop (1) will be the same as for smaller droplet (2) will be half of that for smaller droplet (3) will be one-fourth of that for smaller droplet (4) will be twice of that for smaller droplet

Two glass plates are separated by water. If surface tension of water is 75 dyn/cm and the area of each plate wetted by water is \(8 \mathrm{~cm}^{2}\) and the distance between the plates is \(0.12 \mathrm{~mm}\), then the force applied to separate the two plates is (1) \(10^{2}\) dyn (2) \(10^{4} \mathrm{dyn}\) (3) \(10^{5} \mathrm{dyn}\) (4) \(10^{6} \mathrm{dyn}\)

The angle of contact between glass and water is \(0^{\circ}\) and water (surface tension \(70 \mathrm{dyn} / \mathrm{cm}\) ) rises in a glass capillary up to \(6 \mathrm{~cm}\). Another liquid of surface tension \(140 \mathrm{dyn} / \mathrm{cm}\), angle of contact \(60^{\circ}\) and relative density 2 will rise in the same capillary up to (1) \(12 \mathrm{~cm}\) (2) \(24 \mathrm{~cm}\) (3) \(3 \mathrm{~cm}\) (4) \(6 \mathrm{~cm}\)

Viscous force is somewhat like friction as it opposes, the motion and is non- conservative but not exactly so, because (1) it is velocity dependent while friction is not (2) it is velocity independent while friction is (3) it is temperature dependent while friction is not (4) it is independent of area is like surface tension while friction is dependent

The direction of the excess pressure in the meniscus of a liquid of angle of contact \(2 \pi / 3\) is (1) upward (3) horizontal (2) downward (4) cannot be determined

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