Download Two-dimensional Motion

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Velocity-addition formula wikipedia , lookup

Routhian mechanics wikipedia , lookup

Relativistic quantum mechanics wikipedia , lookup

Kinematics wikipedia , lookup

Inertia wikipedia , lookup

Classical central-force problem wikipedia , lookup

Seismometer wikipedia , lookup

Newton's laws of motion wikipedia , lookup

Centripetal force wikipedia , lookup

Equations of motion wikipedia , lookup

Transcript
Two-dimensional Motion
Introduction
One of Galileo’s greatest insights was that motion in two dimensions may be broken down into
horizontal and vertical motion. This process is the resolution of motion into its components. Galileo noted, in
his early work on kinematics, that an object would continue in motion in a horizontal direction unless and until
some force acted upon it. He also noted that gravity would cause an object to undergo uniform acceleration in
the downward direction. We investigated the downward motion in the lab exercise on the T2 law. In this lab
we couple that uniformly accelerated vertical motion with a horizontal motion at a constant velocity and show
that the motion is parabolic.
Theory
The vertical motion of an object in a uniform gravitational field is described by Equations (1) and (2).
Vy = Voy - gT
(1)
2
y = yo + VoyT = (g/2)T
(2)
In these two equations Vy is the object’s velocity in the y-direction at time T, Voy is the initial velocity of
the object in the y-direction, y is the position of the object at time T, yo is the initial position of the object in the
y-direction, and g is the magnitude of the acceleration of gravity, usually taken to be 9.8 m/s2.
Let us consider the motion of an object starting a distance H above the floor and released from rest. The
noun “rest” implies that Voy is zero. The initial position of the object is H. When the object hits the floor its
final position is zero. The time taken for the object to fall to the floor is found using Equation (2).
0 = H + (0)T - (g/2)T2
(3)
T = (2H/g)1/2
(4)
If we roll a ball off the top of a table of height H it strikes the ground in a time T given by Equation (4).
If the ball has a horizontal velocity Vx as it leaves the table that horizontal velocity is unchanged as the object
falls to the floor. The motion of the object in the horizontal direction is given by Equation (5).
x = xo + VoxT
(5)
If the initial position xo of the object is zero and the position of the object when it hits the floor is R, as
shown in Figure 1, Equation (5) may be written as
R = VoxT
(6)
Notes For success
Experiment
We wish to give the ball a reproducible velocity in the experiment so we construct a ramp from two
pieces of aluminum C-channel. The ramp is constructed by fitting the narrower C-channel into the wider one
about 15 centimeters, or six inches for fans of American units, from the end of the wider piece. Legs are
attached to the wider piece, and these legs are taped to the table top with short pieces of painter’s tape. Four
wooden blocks are used to raise the end of the narrower ramp. For the sake of stability it is best to rest these
blocks on the table at the end of the horizontal piece. One end of the horizontal ramp should overhang the edge
of the table by a few centimeters.
Care must be taken during the experiment so that the ramp does not move.
A piece of white paper is taped with painter’s tape to the floor below the point where the ramp
overhangs the table. A plumb bob, consisting of a ¾”-10 machine nut on a string, is used to mark the point on
the paper directly below the point at which the ball leaves the ramp.
A steel ball is released from a point on the ramp directly above the wooden blocks. The release point
should be marked with tape so that it is the same for all trials. The lab group notes the spot where the ball hits
the floor and extends sheets of paper that are taped to the first sheet of paper to the impact point and slightly
beyond it.
A piece of carbon paper is placed shiny side down so that it is centered on the impact point. DO NOT
tape the carbon paper to the white paper on the floor.
The ball is released down the ramp five times, making five marks on the sheet taped to the floor.
Analysis
Using the equation, x = Vit + ½at2, and the appropriate measurements calculate the time(t) required for
the ball to fall to the floor.
Next, using the time(t) you just calculated and the five impact measurements calculate the velocity of
the ball in the x-direction.
Calculation of Vix is 60% of the lab grade.
Now, the lab group is given a cup from the instructor, and the lab group must calculate where to put the cup so
that the steel ball goes into the cup. The lab group has only one attempt to get the ball into the cup. Of the
remaining 40% of the lab grade, 20% is for the correct calculation of the placement of the cup, 20% is for
actually getting the ball into the cup. The lab group has only one attempt to get the ball into the cup.
Calculation of Vix is 60% of the lab grade.
Diagram (remember there is a difference between a diagram and picture) (2pt)
“the box” w/ correct units (2pts)
Starting equation, filled in equation, work, answer for time(t) (4pts)
Starting equation, filled in equation, work, answer for Vix
(4pts)
The remaining 40% are obtained by solving a ballistics problem.
New Diagram w/ cup (1pt)
“the box” w/ correct units (1pt)
Starting equation, filled in equation, work, answer for time(t) (1pt)
Starting equation, filled in equation, work, answer for your new range. (1pt)
Ball falls into the cup!!! (4pts)
Box 1
Measure the height of the ramp.
Measure the range of the marble.
Calculate the time.
Calculate the velocity in the x-direction.
Box 2
Measure the height of the cup.
Subtract from the height of the ramp.
Calculate the time.
Calculate the range.
Place cup on the calculated range.
Roll marble into the cup.