A piston \(113 \mathrm{~mm}\) diameter and \(150 \mathrm{~mm}\) long has a mass of \(9 \mathrm{~kg}\). It is placed in a vertical cylinder \(115 \mathrm{~mm}\) diameter containing oil of dynamic viscosity \(0.12 \mathrm{~Pa} \cdot \mathrm{s}\) and relative density \(0.9\) and it falls under its own weight. Assuming that piston and cylinder are concentric, calculate the time taken for the piston to fall steadily through \(75 \mathrm{~mm}\).

Short Answer

Expert verified
Time taken is approximately 0.0054 s.

Step by step solution

01

Convert Units to SI

Convert all given measurements to SI units for consistent calculations.- Diameter of the piston: 113 mm = 0.113 m- Length of the piston: 150 mm = 0.150 m- Diameter of the cylinder: 115 mm = 0.115 m- Distance of fall: 75 mm = 0.075 m
02

Calculate the Clearance

Calculate the clearance between the piston and the cylinder.Clearance, \[ h_c = \frac{0.115 - 0.113}{2} = 0.001 m \]
03

Calculate the Force Due to Gravity

Calculate the force acting on the piston due to its weight.Where: - Mass \( m = 9 \text{ kg} \)- Gravity \( g = 9.81 \text{ m/s}^2 \)Force, \[ F_g = m \cdot g = 9 \cdot 9.81 = 88.29 \text{ N} \]
04

Calculate the Viscous Drag Force

Use the dynamic viscosity and clearance to determine the viscous drag force.Where: - Dynamic viscosity \( \mu = 0.12 \text{ Pa} \cdot \text{s} \)- Velocity \( v \)- Surface area \( A = \pi \cdot d_l \cdot L_p = \pi \cdot 0.113 \cdot 0.150 = 0.0531 \text{ m}^2 \)Viscous force \[ F_v = \mu \cdot \frac{v}{h_c} \cdot A = 0.12 \cdot \frac{v}{0.001} \cdot 0.0531 = 6.372 \cdot v \text{ N} \]
05

Establish the Steady-State Condition

At steady state, gravitational force is balanced by the viscous force.\[ F_g = F_v \Longrightarrow 88.29 = 6.372 \cdot v \]Hence, solve for velocity:\[ v = \frac{88.29}{6.372} = 13.86 \text{ m/s} \]
06

Calculate the Time Taken to Fall 75 mm

Use the velocity to calculate the time taken to fall through a distance of 75 mm.\[ t = \frac{d}{v} = \frac{0.075}{13.86} \approx 0.0054 \text{ s} \]

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Key Concepts

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

dynamic viscosity
Dynamic viscosity is a measure of a fluid's resistance to flow. It describes how much resistance a fluid offers when subjected to shear stress. Higher viscosity means the fluid is thicker and flows less easily. In our exercise, the oil in the cylinder has a dynamic viscosity of 0.12 Pa·s. This tells us how sticky or thick the oil is, which directly affects how it will slow down the falling piston. For engineers and students, it's crucial to understand how viscosity impacts movement in fluid mechanics problems. The unit for dynamic viscosity in the SI system is Pascal-seconds (Pa·s). When calculating forces in fluid dynamics, remember to incorporate viscosity since it significantly influences the final results.
gravitational force
Gravitational force is the force exerted by gravity on an object. It is calculated as the product of the object's mass and gravitational acceleration. In this exercise, the piston with a mass of 9 kg falls under its weight, experiencing a gravitational pull. We used the formula \( F_g = m \cdot g \) to find it. Substituting in the values, we get \( F_g = 9 \cdot 9.81 = 88.29 \ \text{N} \). This force drives the piston downward, where it is then counteracted by the viscous force of the oil. Understanding gravitational force helps in predicting how objects will move when falling, which is essential in fluid mechanics and other physics-related fields.
steady-state condition
A steady-state condition occurs when all forces acting on an object are balanced, resulting in constant velocity. In our problem, the piston reaches steady state when gravitational force is equal to the viscous drag force exerted by the oil. We establish this condition with the equation \( F_g = F_v \). Both forces being equal means there is no acceleration, just consistent falling speed. The concept of steady-state is vital in many engineering and physics scenarios because it simplifies the analysis by indicating a stable situation without acceleration. Understanding this condition helps predict system behavior under long-term operation.
clearance calculation
Clearance refers to the gap or spacing between two components. In this exercise, clearance is the space between the piston and the cylinder wall. It's calculated to consider how oil flows in the gap, affecting the viscous force. We use the formula: \( h_c = \frac{0.115 - 0.113}{2} = 0.001 \ \text{m} \). This small gap significantly influences the calculations for viscous drag. In fluid mechanics, precise clearance measurements are crucial because even slight changes can impact the resistance force drastically, affecting the system's performance.
SI unit conversion
SI unit conversion ensures consistency and accuracy in scientific calculations. Converting measurements to SI units (meters, kilograms, seconds) helps standardize the values across all steps. For example, in our exercise, we converted diameters from millimeters to meters (113 mm to 0.113 m). This makes the subsequent calculations more straightforward and prevents errors. Always make sure to convert units at the beginning to avoid confusion and ensure that all formulas and constants align properly. Using SI units is essential in engineering and science for seamless communication and comparison of data worldwide.

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Most popular questions from this chapter

A cylindrical drum of length \(l\) and radius \(r\) can rotate inside a fixed concentric cylindrical casing, the clearance space \(c\) between the drum and the casing being very small and filled with liquid of dynamic viscosity \(\mu\). To rotate the drum with angular velocity \(\omega\) requires the same power as to pump the liquid axially through the clearance space while the drum is stationary, and the pressure difference between the ends of the drum is \(p .\) The motion in both cases is laminar. Neglecting end effects, show that $$ p=\frac{2 \mu \operatorname{lr} \omega \sqrt{3}}{c^{2}} $$

A steel sphere, \(1.5 \mathrm{~mm}\) diameter and of mass \(13.7 \mathrm{mg}\), falls steadily in oil through a vertical distance of \(500 \mathrm{~mm}\) in \(56 \mathrm{~s}\). The oil has a density of \(950 \mathrm{~kg} \cdot \mathrm{m}^{-3}\) and is contained in a drum so large that any wall effects are negligible. What is the viscosity of the oil? Verify any assumptions made.

A plane bearing plate is traversed by a very wide, \(150 \mathrm{~mm}\) long, plane inclined slipper moving at \(1.5 \mathrm{~m} \cdot \mathrm{s}^{-1}\). The clearance between slipper and bearing plate is \(0.075 \mathrm{~mm}\) at the toe and \(0.025 \mathrm{~mm}\) at the heel. If the load to be sustained by the bearing divided by the width is \(500 \mathrm{kN} \cdot \mathrm{m}^{-1}\), determine the viscosity of the lubricant required, the power consumed divìded by the width of the bearing, the maximum pressure in the lubricant and the position of the centre of pressure.

Two circular plane discs of radius \(R_{2}\) have their axes vertical and in line. They are separated by an oil film of uniform thickness. The oil is supplied continuously at a pressure \(p_{1}\) to a well of radius \(R_{1}\) placed centrally in the lower disc, from where it flows radially outwards and escapes to atmosphere. The depth of the well is large compared with the clearance between the discs. Show that the total force tending to lift the upper disc is given by $$ \frac{\pi p_{1}\left(R_{2}^{2}-R_{1}^{2}\right)}{2 \ln \left(R_{2} / R_{1}\right)} $$ and determine the clearance when the dynamic viscosity of the oil is \(0.008 \mathrm{~Pa} \cdot \mathrm{s}\), the flow \(0.85 \mathrm{~L} \cdot \mathrm{s}^{-1}, p_{1}=550 \mathrm{kPa}, R_{1}=\) \(12.5 \mathrm{~mm}\) and \(R_{2}=50 \mathrm{~mm}\). Assume laminar flow and neglect end effects.

Show that when laminar flow occurs with mean velocity \(u_{\mathrm{m}}\) between extensive stationary flat plates the mean kinetic energy divided by mass of the fluid is \(1.543 u_{\mathrm{m}}^{2} / 2\).

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