Equipment: Ballistic pendulum, carbon paper, meter stick, clamp box, triple beam balance, plumb.
Introduction: In this experiment a steel ball will be shot into the bob of a pendulum and the height, h, to which the pendulum bob moves, as shown in Figure 1, will determine the initial velocity, V, of the bob after it receives the moving ball.
Figure 1:
If we equate the kinetic energy of the bob and ball at the bottom to the potential energy of the bob and ball at the height, h, that they are raised to, we get:
(K.E)bottom = (P.E)top
1/2( M+m) V^2 = ( M+m) gh
Where M is the mass of the pendulum and m is the mass of the ball. Solving for V we get:
V = √(2gh) ----------(1)
Using conservation of momentum we know the momentum before impact (collision) should be the same as the momentum after impact. Therefore:
pf = pi
or
mvo= (M+m)V -----------(2)
Where vo is the initial velocity of the ball before impact. By using equations (1) and (2) we can therefore find the initial velocity, vo, of the ball.
We can also determine the initial velocity f the ball by shooting the ball as above but this time allowing the ball to miss the pendulum bob and travel horizontally under the influence of gravity. In this case we simply have a projectile problem where we cam measure the distance traveled horizontally and vertically (see Figure 2) and then determine the initial velocity, vo, of the ball.
Figure 2:
Starting with equations:
△x = voxt + 1/2axt^2 -------------(3)
△y = voyt + 1/2ayt^2 -------------(4)
You should be able to derive the initial velocity of the ball in the horizontal direction (assuming that and known).
Part I: Determination of initial velocity from conservation of energy
1. Set the apparatus near one edge of the table as shown in figure 2. Make sure that the base is accurately horizontal, as shown by a level. Clamp the frame to the table. To make the gun ready for shooting, rest the pendulum on the rack, put the ball in position on the end of the rod and, holding the base with one hand, pull back on the ball with the other until the collar on the rod engages the trigger. This compresses the spring a definite amount, and the ball is given the same initial velocity every time the gun is shot.
2. Release the pendulum from the rack and allow it to hang freely. When the pendulum is at rest, pull the trigger, thereby propelling the ball into the pendulum bob with a definite velocity. This causes the pendulum to swing from a vertical position to an inclined position with the pawl engaged in some particular tooth of the rack.
3. Shoot the ball into the cylinder about nine times, recording each point on the rack at which the pendulum comes to rest. This in general will not be exactly the same for all cases but may vary by several teeth of the rack. The mean of these observation gives the mean highest position of the pendulum. Raise the pendulum until its pawl is engaged in the tooth corresponding most closely to the mean value and measure h1, the elevation above the surface of the base of the base of the index point for the center of gravity. Next release the pendulum and allow it to hang in its lower most position and measure h2. The difference between these two values gives h, the vertical distance through which the center of gravity of the system is raised after shooting the ball.
Record h:
Our average point on the rack is 12.9, which corresponds to 12.3cm
So, h1= 12.3cm
We measured h2 = 3.8cm
h= h2 - h1= 12.3cm- 3.8cm= 8.5cm
4. Carefully remove the pendulum from its support. Weigh and record the masses of the pendulum and of the ball. Replace the pendulum and carefully adjust the thumb screw.
M (mass of pendulum) = 194g
m ( mass of the ball) = 56.8g
5. From the data calculate the initial velocity v using equations (1) and (2).
Because:
V = √(2gh)
mvo= (M+m)V
So:
vo= (M+m) ×√(2gh) / m
= (194+56.8) ×√(2×9.8×0.085) / 56.8
= 5.7 m/s
Part II: Determination of initial velocity from measurements of range and fall
1. To obtain the data for this part of the experiment the pendulum is positioned up on the rack so that it will not interfere with the free flight of the ball. One observer should watch carefully to determine the point at which the ball strikes the floor. The measurements in this part of the experiment are made with reference to this point and the point of departure of the ball. Clamp the frame to the table. as it is important that the apparatus not be moved until the measurements have been completed. A piece of paper taped to the floor at the proper place and cover with carbon paper will help in the exact determination of the spot at which the ball strikes the floor.
2. Shoot the ball a number of times, nothing each time the point at which it strikes the floor. Determine, relative to the edge of the paper, the average position of impact of the ball. Determine the distances △x and △y calculate vo by the use of equations (3) and (4). Make careful stretches in your lab report show all of the distances involved.
The distance from the ball to the paper: 258.4cm
The distance of the ball on the paper: 17.4cm
The distance of the ball on the paper |
△y(height) = 99.7cm
△y = voyt + 1/2ayt^2
0.997 = 0 + (1/2) × 9.8 × t^2
t = 0.45s
△x = voxt + 1/2axt^2
2.76 = vo × 0.45 +0
vo = 6.1 m/s
Percent of difference between part I and part II:
(6.1-5.7) / [(6.1+5.7) /2] = 6.8%
Conclusion:
What you learned
After doing this Ballistic Pendulum lab, I learned that the momentum and energy of the of the ball and pendulum's system are both conserved if there is no external forces. We used the the law of conservation of momentum and conservation of energy to find the initial velocity of the ball, and then compare to the value we got from measurement of range and fall. We found these two values are really close, which proves the law of conservation of momentum and conservation of energy.
Source of error:
1. The table is not exactly horizontal, so our h is not accurate.
2. The friction of the system and the air resistance are external forces that can't be avoided, which will lose the energy of the system.
Which method did you think was more accurate? Explain.
The method 1 will be more accurate.
Although in both method 1 and method 2, we assume that there is no external forces, the friction and air resistance still can't be avoided. But in method 2, the ball will go through the air for a long time that will be influenced by air resistance more than method 1.
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