/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 75 The viscous force on an oil drop... [FREE SOLUTION] | 91Ó°ÊÓ

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The viscous force on an oil drop is measured to be equal to \(3.0 \times 10^{-13} \mathrm{~N}\) when the drop is falling through air with a speed of \(4.5 \times 10^{-4} \mathrm{~m} / \mathrm{s}\). If the radius of the drop is \(2.5 \times 10^{-6} \mathrm{~m}\), what is the viscosity of air?

Short Answer

Expert verified
The viscosity of air is \(1.69 \times 10^{-5} \, \mathrm{Pa} \, \mathrm{s}\).

Step by step solution

01

Understand the problem

The task is to determine the viscosity of air based on the viscous force acting on an oil droplet, the speed at which the droplet is falling, and the radius of the droplet. Stokes' law is used, which states that the force of viscosity \(F\) is equal to \(6 \pi \eta r v\), where \(\eta\) is the viscosity, \(r\) is the radius of the droplet and \(v\) is the velocity.
02

Calculate viscosity

To solve for viscosity \(\eta\), need to rearrange the formula of Stokes' law to: \(\eta = F / (6 \pi r v)\). Here, \(F = 3 \times 10^{-13}\) N, \(r = 2.5 \times 10^{-6}\) m, and \(v = 4.5 \times 10^{-4}\) m/s. By substituting these values into the formula, we can calculate \(\eta\).
03

Substitute the values into the formula

The values can now be inserted into the formula like so: \(\eta = (3.0 \times 10^{-13}) / (6 \pi \times 2.5 \times 10^{-6} \times 4.5 \times 10^{-4})\).
04

Compute the final value

By performing the calculations, the viscosity of air \(\eta\) is found to be \(1.69 \times 10^{-5} \, \mathrm{Pa} \, \mathrm{s}\).

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Key Concepts

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

Viscosity of Air
Viscosity, often described as the "thickness" of a fluid, refers to its resistance to flow. When we talk about the viscosity of air, we are referring to how resistant air is to motion or how "sticky" it behaves when particles move through it. Unlike liquids, air is a gas, and its viscosity is relatively much lower.

In our everyday experience, air feels easy to move through and doesn't offer much resistance. However, for very small particles like oil droplets, air's viscosity is significant enough to influence their movement. This property becomes crucial in fields like aerodynamics and meteorology.

Factors influencing air viscosity include temperature and pressure. Generally, as the temperature increases, the viscosity of air also increases because molecules move more vigorously, affecting the flow resistance.
Viscous Force
Viscous force is a type of friction that occurs in fluids. When an object moves through a fluid, such as air or oil, the fluid molecules exert a force opposing this motion, known as the viscous force. This force depends on how quickly the object moves, its size, and the fluid's viscosity.

Stokes' Law helps to determine this force quantitatively for small spherical objects (like our oil drop) moving through a viscous fluid. The law gives the formula for viscous force as:
  • \( F = 6 \pi \eta r v \), where:
  • \( F \) is the viscous force,
  • \( \eta \) is the fluid's viscosity,
  • \( r \) is the radius of the spherical object, and
  • \( v \) is the object's velocity through the fluid.
Understanding viscous force is key for designing efficient systems in engineering and technology, such as automotive and aerospace components, where fluid interactions constantly occur.
Calculation of Viscosity
The calculation of viscosity is crucial for understanding how fluids behave, especially in engineering and physical sciences. Using Stokes' Law, we can determine the viscosity of a fluid by measuring the viscous force acting on a moving object, like our given oil drop.

In the example problem, we rearranged Stokes' formula to solve for viscosity \( \eta \):
  • \( \eta = \frac{F}{6 \pi r v} \)
Given the values:
  • Force \( F = 3.0 \times 10^{-13} \) N,
  • Radius \( r = 2.5 \times 10^{-6} \) m, and
  • Velocity \( v = 4.5 \times 10^{-4} \) m/s,
we substitute these into the equation:
  • \( \eta = \frac{3.0 \times 10^{-13}}{6 \pi \times 2.5 \times 10^{-6} \times 4.5 \times 10^{-4}} \)
Finally, performing the calculations helps us ascertain the viscosity of air is approximately \( 1.69 \times 10^{-5} \, \mathrm{Pa} \, \mathrm{s} \). This result is essential in predicting how objects will behave when moving through the air.

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Most popular questions from this chapter

A spherical weather balloon is filled with hydrogen until its radius is \(3.00 \mathrm{~m}\). Its total mass including the instruments it carries is \(15.0 \mathrm{~kg}\). (a) Find the buoyant force acting on the balloon, assuming the density of air is \(1.29 \mathrm{~kg} / \mathrm{m}^{3}\). (b) What is the net force acting on the balloon and its instruments after the balloon is released from the ground? (c) Why does the radius of the balloon tend to increase as it rises to higher altitude?

The total cross-sectional area of the load-bearing calcified portion of the two forearm bones (radius and ulna) is approximately \(2.4 \mathrm{~cm}^{2}\). During a car crash, the forearm is slammed against the dashboard. The arm comes to rest from an initial speed of \(80 \mathrm{~km} / \mathrm{h}\) in \(5.0 \mathrm{~ms}\). If the arm has an effective mass of \(3.0 \mathrm{~kg}\) and bone material can withstand a maximum compressional stress of \(16 \times 10^{7} \mathrm{~Pa}\), is the arm likely to withstand the crash?

Water flowing through a garden hose of diameter \(2.74 \mathrm{~cm}\) fills a \(25.0\) - L bucket in \(1.50 \mathrm{~min}\). (a) What is the speed of the water leaving the end of the hose? (b) A nozzle is now attached to the end of the hose. If the nozzle diameter is one-third the diameter of the hose, what is the speed of the water leaving the nozzle?

In a water pistol, a piston drives water through a larger tube of radius \(1.00 \mathrm{~cm}\) into a smaller tube of radius \(1.00 \mathrm{~mm}\) as in Figure \(\mathrm{P} 9.51\). (a) If the pistol is fired horizontally at a height of \(1.50 \mathrm{~m}\), use ballistics to determine the time it takes water to travel from the nozzle to the ground. (Neglect air resistance and assume atmospheric pressure is \(1.00 \mathrm{~atm}\).) (b) If the range of the stream is to be \(8.00 \mathrm{~m}\), with what speed must the stream leave the nozzle? (c) Given the areas of the nozzle and cylinder, use the equation of continuity to calculate the speed at which the plunger must be moved. (d) What is the pressure at the nozzle? (e) Use Bernoulli's equation to find the pressure needed in the larger cylinder. Can gravity terms be neglected? (f) Calculate the force that must be exerted on the trigger to achieve the desired range. (The force that must be exerted is due to pressure over and above atmospheric pressure.)

The human brain and spinal cord are immersed in the cerebrospinal fluid. The fluid is normally continuous between the cranial and spinal cavities and exerts a pressure of 100 to \(200 \mathrm{~mm}\) of \(\mathrm{H}_{2} \mathrm{O}\) above the prevailing atmospheric pressure. In medical work, pressures are often measured in units of \(\mathrm{mm}\) of \(\mathrm{H}_{2} \mathrm{O}\) because body fluids, including the cerebrospinal fluid, typically have nearly the same density as water. The pressure of the cerebrospinal fluid can be measured by means of a spinal tap. A hollow tube is inserted into the spinal column, and the height to which the fluid rises is observed, as shown in Figure P9.83. If the fluid rises to a height of \(160 \mathrm{~mm}\), we write its gauge pressure as \(160 \mathrm{~mm} \mathrm{H}_{2} \mathrm{O}\). (a) Express this pressure in pascals, in atmospheres, and in millimeters of mercury. (b) Sometimes it is necessary to determine whether an accident victim has suffered a crushed vertebra that is blocking the flow of cerebrospinal fluid in the spinal column. In other cases, a physician may suspect that a tumor or other growth is blocking the spinal column and inhibiting the flow of cerebrospinal fluid. Such conditions can be investigated by means of the Queckensted test. In this procedure the veins in the patient's neck are compressed, to make the blood pressure rise in the brain. The increase in pressure in the blood vessels is transmitted to the cerebrospinal fluid. What should be the normal effect on the height of the fluid in the spinal tap? (c) Suppose compressing the veins had no effect on the level of the fluid. What might account for this phenomenon?

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