/*! 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 50 A block of mass \(M\) slides on ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A block of mass \(M\) slides on a thin film of oil. The film thickness is \(h\) and the area of the block is \(A\). When released, mass \(m\) exerts tension on the cord, causing the block to accelerate. Neglect friction in the pulley and air resistance. Develop an algebraic expression for the viscous force that acts on the block when it moves at speed \(V\). Derive a differential equation for the block speed as a function of time. Obtain an expression for the block speed as a function of time. The mass \(M=5 \mathrm{kg}, m=1 \mathrm{kg}, A=25 \mathrm{cm}^{2},\) and \(h=0.5 \mathrm{mm} .\) If it takes \(1 \mathrm{s}\) for the speed to reach \(1 \mathrm{m} / \mathrm{s}\), find the oil viscosity \(\mu .\) Plot the curve for \(V(t)\).

Short Answer

Expert verified
The equation for the force on the block is \((M+m) a = M g - \mu * A * V / h)\). The differential equation for speed is \((M+m) dv/dt = M g - \mu * A * V / h)\). The solution to this differential equation is \(V(t) = (Mg / \mu A / h) (1 - e^{-(\mu * A / h ) * t / M + m} )\). After solving for \(\mu\), we can plot the speed function \(V(t)\).

Step by step solution

01

Determine the Force on the Block

First, let's resolve the forces on the block. The gravity of block \(M\) pulls downwards with force \(Mg\). The tension in the string due to mass \(m\) pulls in the opposite direction with force \(mg\). As the block moves through the oil, it experiences a viscous force \(F\), given by the formula \(F = \mu * A * V / h\), where \(\mu\) is the viscosity of the oil, \(A\) is the contact area, \(V\) is the speed, and \(h\) is the oil film thickness.
02

Create a Differential Equation for Speed

Now, let's balance the forces according to Newton's second law \(F = ma\). The acceleration \(a\) can be substituted as \(dv/dt\), where \(v\) is the velocity and \(t\) is time. This gives the equation: \((M+m) a = M g - \mu * A * V / h)\), which simplifies to: \((M+m) dv/dt = M g - \mu * A * V / h)\), which is our differential equation for speed.
03

Solve the Differential Equation

Separate and integrate the differential equation. By doing so, the following expression for speed can be found: \(V(t) = (Mg / \mu A / h) (1 - e^{-(\mu * A / h ) * t / M + m} )\).
04

Find the Oil Viscosity

To find the oil viscosity, take the given condition: it takes 1 second to reach a speed of 1 m/s. Substituting these values and the given constants into the speed expression, one can solve for \(\mu\).
05

Plotting the Speed Function

The function \(V(t)\) can now be plotted over a reasonable range of time values using any graphing software. The function will show exponential growth, reaching an asymptote at \(V = \frac{Mg}{\mu A/h}\)

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

An insulation company is examining a new material for extruding into cavities. The experimental data is given below for the speed \(U\) of the upper plate, which is separated from a fixed lower plate by a 1 -mm-thick sample of the material, when a given shear stress is applied. Determine the type of material. If a replacement material with a minimum yield stress of \(250 \mathrm{Pa}\) is needed, what viscosity will the material need to have the same behavior as the current material at a shear stress of \(450 \mathrm{Pa} ?\) $$\begin{array}{ccccccccccc}\tau(P a) & 50 & 100 & 150 & 163 & 171 & 170 & 202 & 246 & 349 & 444 \\ U(\mathrm{m} / \mathrm{s}) & 0 & 0 & 0 & 0.005 & 0.01 & 0.025 & 0.05 & 0.1 & 0.2 & 0.3 \end{array}$$

The flow field for an atmospheric flow is given by \\[\vec{V}=-\frac{K y}{2 \pi\left(x^{2}+y^{2}\right)} \hat{i}+\frac{K x}{2 \pi\left(x^{2}+y^{2}\right)}\\] where \(K=10^{5} \mathrm{m}^{2} / \mathrm{s},\) and the \(x\) and \(y\) coordinates are parallel to the local latitude and longitude. Plot the velocity magnitude along the \(x\) axis, along the \(y\) axis, and along the line \(y=x,\) and discuss the velocity direction with respect to these three axes. For each plot use a range \(x\) or \(y=-1 \mathrm{km}\) to \(1 \mathrm{km}\), excluding \(\mathrm{L} x\) I or \(|y|<100 \mathrm{m} .\) Find the equation for the streamlines and sketch several of them. What does this flow field model?

A concentric-cylinder viscometer is shown. Viscous torque is produced by the annular gap around the inner cylinder. Additional viscous torque is produced by the flat bottom of the inner cylinder as it rotates above the flat bottom of the stationary outer cylinder. Obtain an algebraic expression for the viscous torque due to flow in the annular gap of width \(a\). Obtain an algebraic expression for the viscous torque due to flow in the bottom clearance gap of height \(b\). Prepare a plot showing the ratio, \(b / a,\) required to hold the bottom torque to 1 percent or less of the annulus torque, versus the other geometric variables. What are the design implications? What modifications to the design can you recommend?

Streaklines are traced out by neutrally buoyant marker fluid injected into a flow ficld from a fixed point in space. A particle of the marker fluid that is at point \((x, y)\) at time \(t\) must have passed through the injection point \(\left(x_{0}, y_{0}\right)\) at some earlier instant \(t=\tau .\) The time history of a marker particle may be found by solving the pathline equations for the initial conditions that \(x=x_{0}, y=y_{0}\) when \(t=\tau .\) The present locations of particles on the streakline are obtained by setting \(\tau\) equal to values in the range \(0 \leq \tau \leq t\). Consider the flow ficld \(\vec{V}=a x(1+b t) \hat{i}+c y \hat{j},\) where \(a=c=1 \mathrm{s}^{-1}\) and \(b=0.2 \mathrm{s}^{-1}\). Coordinates are measured in meters. Plot the streakline that passes through the initial point \(\left(x_{0}, y_{0}\right)=(1,1),\) during the interval from \(t=0\) to \(t=3\) s. Compare with the streamline plotted through the same point at the instants \(t=0,1,\) and \(2 \mathrm{s}\).

A flow field is given by \(\vec{V}=A x i+2 A y\), where \(A=2 s^{-1}\) Verify that the parametric equations for particle motion are given by \(x_{p}=c_{1} e^{A t}\) and \(y_{p}=c_{2} e^{2 u_{l}} .\) Obtain the equation for the pathline of the particle located at the point \((x, y)=(2,2)\) at the instant \(t=0 .\) Compare this pathline with the streamline through the same point.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.