Lab 3

Motion under the influence of a constant force

Newton's second law, F = ma, predicts the future motion of an object if we know its initial motion and the net force that is acting on the object.  Today you will explore this motion when the net force is approximately constant.

Equipment needed:

Open a Microsoft Word document to keep a log of your experimental procedures and your results.  This log will form the basis of your studio session report.  Address the points highlighted in blue.  Answer all questions.


Free-fall - The acceleration of gravity

Gravity is the force of nature we are most aware of.  One can argue that other forces, such as the electromagnetic force, which holds molecules together in solid objects, or nuclear forces, which determine the structure of atoms, are more important, but these forces are less obvious to us.  Near the surface of Earth the force of gravity on an object of mass m equals Fg = mg.  It is constant and points straight down.  If we can neglect other forces and the net force is approximately equal to Fg, then we have motion with constant acceleration g.

Observation

Hold a tennis ball at about your height and then let go.  Observe the motion of the ball.

Describe the motion as the ball is falling.

Experiment 1

It does not take the ball a long time to reach the floor.  It is hard to get detailed information about its motion without using external measuring instruments.  In this experiment, the instrument is a video camera.  You will analyze a video clip.  The clip shows a ball being dropped.  You will determine the position of the freely-falling ball as a function of time by stepping through the video clip frame-by-frame and by reading the time and the position coordinates of the ball off each frame.  You will construct a spreadsheet with columns for time and position and use this spreadsheet to find the velocity as a function of time.  The slope of a velocity versus time graph yields the acceleration of the ball.

Procedure:

To play the video clip or to step through it frame-by-frame click the "Begin" button.


Produce a graph of position versus time.  Label the axes.

Let us find the velocity of the ball as a function of time.  We find vy =  ∆y/∆t by dividing the difference in successive position by the difference in the times the ball was at those positions.

Produce a graph of velocity versus time. Label the axes.

For motion with constant acceleration we expect that y changes as a function of time as y = y0 + v0t + ½at2, where a is the acceleration. For an object accelerating at a constant rate g we have y = y0 + v0t + ½gt2, so y as a function of t is a polynomial of order 2 (a section of a parabola).  We can reduce numerical errors in finding the acceleration of the ball by fitting our position versus time data directly with a polynomial of order 2.


Projectile motion

Experiment 2

A ball is moving in two dimensions under the influence of a constant gravitational force.  It is hard to get detailed information about its motion without using external measuring instruments.  In this experiment, the instrument is a video camera.  You will analyze a video clip.  The clip shows a ball being thrown.  You will determine the position of the ball in two dimensions as a function of time by stepping through the video clip frame-by-frame and by reading the time and the position coordinates of the ball off each frame.  You will construct a spreadsheet with columns for time and position and use this spreadsheet to find the x and y component of the velocity as a function of time.

Procedure:

To play the video clip or to step through it frame-by-frame click the "Begin" button.


Produce graphs of the x and y components of position versus time.  Label the axes.

Paste your graphs with trendlines into your log.


Measuring the coefficients of static friction

In this experiment you will measure the coefficient of static friction for a wood block and a felt-covered block in contact with a metal track.  The surface of the track makes an angle θ with the horizontal.  For angles θ > θmax the block will accelerate down the sloping track.

You will determine the angle θmax for which the maximum force of static friction fs_max = μsN = μsmg cosθmax just cancels the component of the gravitational force fg = mg sinθmax pointing down the track.  You will then solve for the coefficient of static friction μs.

Experiment 3

Find the coefficient of static friction.

Pictures of the track and the wood block are shown below.  The block has a mass of 112.4 g and one side of the block is covered with felt.  A horizontal and a vertical meter stick are taped to the wall behind the track and can be used to calibrate the video clips.

image     image

 

To play or step through the video clips frame-by-frame click the buttons below.







Construct a table as shown below.  Insert this table into your log.

surface θmax (deg) μs
wood    
felt    

Comment on your results.  Explain how you measured the angle θmax.


Convert your log into a lab report.

Name:
E-mail address:

Laboratory 3 Report

Save your Word document (your name_lab3.docx), go to Canvas, Assignments, Lab 3, and submit your document.