Activities on Velocity in Circular Motion

In all of the following Activities, keep all of the applet's eight slider settings fixed at their default values except for that of the time step Dt. Change that as instructed in the Activities.

Activities

  1. Display two vectors: the position vector of the mass point and the velocity vector of the mass point, the latter with its tail end at the mass point (select "velocity at particle" in the Vector Panel). Set the applet to the Continuous mode. Display the position trace (Trace P), but not the velocity trace (Trace V).

    Play the motion, and pause it at several instants. Make a drawing of the mass point's path and of the mass point's position and velocity vectors at the instants when you pause the motion.

    In a sentence or two, characterize how the direction of the velocity vector is related to that of the position vector and how the velocity vector is oriented relative to the mass point's path. Can you confirm the following general statement about the direction of the velocity vector?

    The velocity vector at a given instant points in the direction in which the tip of the position vector is moving at that instant, which is the direction of the tangent to the mass point's path at that instant.

    What do you observe about the magnitude of the velocity vector during the motion?

  2. The purpose of Activity 2 is to obtain an understanding of the general (indented) statement on velocity in Activity 1 that is based solely on the definition of velocity as time-rate-of-change of position.

    Continuing from Activity 1, click Rewind and set the applet to the Incremental mode and the time step to Dt = 0.50 s.

    Use the Step button to take one step into the motion. Make a drawing of the position vectors vector ri and vector rf at the beginning and end of the time step, the displacement vector Dvector r during the time step, and the velocity vectors vector vi and vector vf at the beginning and end of the time step. Estimate the angles between the initial and final velocity vectors and between the displacement and initial velocity vectors.

    In a sentence or two, describe how the direction of the displacement vector is related to those of the initial and final velocity vectors and by how much the directions of all these vectors differ.

    Click Rewind, reduce the time step to Dt = 0.25 s, and again take the first step into the motion. Again, draw all vectors and estimate the angles between the initial and final velocity vectors and between the initial velocity and displacement vectors.

    Again, describe how the direction of the displacement vector compares to those of the initial and final velocity vectors and how the displacement vector during the 0.25-s time step compares to that during the 0.50-s time step.

    Click Replay, and repeat these observations once more for a time step Dt = 0.10 s.

    Velocity is defined as the limit of the ratio Dvector r/Dt as Dt approaches 0. As Dt approaches 0, does the direction of Dvector
r/Dt, which is the same as that of Dvector r, approach the direction of the velocity at the beginning of the time interval?

    The displacement Dvector r forms a cord of the mass point's path. Do you observe that as Dt approaches 0 the direction of the cord approaches that of the tangent to the path at the mass point's initial position?

    In what sense do the observations in Activity 2 confirm the general statement from Activity 1?

    The velocity vector at a given instant points in the direction in which the tip of the position vector is moving at that instant, which is the direction of the tangent to the mass point's path at that instant.
  3. This activity is a repeat of Activity 2 with numbers.

    Continuing from Activity 2, click Rewind, change the step size back to Dt = 0.50 s, and display the Data box. Make sure the applet is still in the Incremental mode and that no other settings have changed.

    Take one step into the motion. Record the values of Dvector r and Dt, and work out the ratio Dvector r/Dt in terms of its x,y scalar components. Compare this ratio to the initial velocity vector vi.

    Using the x,y scalar components of Dvector r/Dt worked out above and the x,y scalar components of vector vi listed in the Data box, draw the two vectors Dvector r/Dt and vector
vi. Draw them with their tail ends joined for better comparison. For better accuracy, you may want to draw the vectors on graph paper.

    As in Activity 2, repeat this with time steps equal to 0.25 s and 0.10 s.

    Does Dvector
r/Dt approach vector vi as the size of the time step decreases?

    The applet will let you choose time steps smaller than Dt = 0.10 s, but the values of Dvector r/Dt will become unreliable as the time step becomes too small because of a loss of significant figures. This is evident visually as well because the displacement vector Dvector r becomes hard to recognize.

  4. Repeat Activities 2 and 3 at a different point of the mass point's path. E.g., after clicking Replay, drag the mass point to a point with phase d = 1 rad. (d is the first item in the Data box). Use this point as the initial point for observations like those in Activities 2 and 3.