CONSERVATION OF MOMENTUM: BALLISTIC PENDULUM CATAPANG, JAMIEL S. 2016142388 PHY01 G-223 SCORE Group Report (40) Analysis (25) Conclusion (25) Presentation (10) Safe Assign Score (30% max) TOTAL Engr. Ericson D. Dimaunahan Instructor October , 2017 ANALYSIS The experiment all throughout was done really quickly. It was finished for like less than an hour, approximately 55 minutes or lesser. The preparation of the experiment was done for almost 10 seconds because it just only needs a pendulum with accessories and a meterstick. There have been no problems encountered in measuring and setting up of the experiment. It is just that when we started recording and gathering data, the ball automatically goes out from the launcher. Also, the ball sometimes do not shoot in the pendulum bob; hence causing the ball to strike anywhere. We had a hard time getting the angles and its average for five trials because of those issues. The design of the experiment, as observed, was particularly manually getting data needed in the experiment. For example, the mass of the steel ball and the mass of the pendulum bob were determined not by solving anything. The initial height of the pendulum bob was also determined through the use of a meterstick. In getting the initial speed of the steel ball (VI), as observed, the momentum (p) is conserved before and after collision, a perfect inelastic collision. Thus, it can be calculated from the mass of the pendulum bob with added mass and the mass of the steel ball. RESULTS Table Summary Mass of the steel ball, m1 = 65.875 g Mass of the pendulum, m2 = 141.7 g W/ 100 g added mass = 241.7 g TRIAL Angle 1 38° 2 36.5° 3 37° 4 37° 5 36.5° Average Angle = 37° Initial height of the pendulum, y1 = 3.2 cm Derived final height of the pendulum, y2 = 9 cm Increase in height, y = y2 – y1 = 5.8 cm HORIZONTAL PROJECTILE Initial height, y* 3.2 cm Average horizontal 45.86 cm distance, x* Initial speed of the steel 49.7820 cm ball (Eq. 4), vI Initial speed of the steel 56.7489 cm ball (Eq. 7), v1 Percent difference for vI 13.0795% DISCUSSION At first, the mass of the steel ball and the mass of the ballistic pendulum were given to be 65.875-g and 141.7-g with added 100-g mass, respectively. The following needed materials were set up with the pendulum bob at 0° level. Then, the researchers measured the initial height (y1) of the pendulum from its base to the reference height, which is the tabletop, that they had used using a meterstick. The steel ball was then fired to the pendulum with the same initial height (y1 = 3.2-cm) and noted the corresponding angle for five times. Its average was calculated, αave = 37°. The vertical distance (y2) was then determined from the base of the ballistic pendulum to the reference height used by manually setting the pendulum bob to the average angle computed (α). The increase in height was later calculated by getting the difference of the initial height (y1) and final height (y2), y = y2 – y1 = 5.8-cm. Since the researchers have determined the increase height (y), the equation no. 4, V I = (m1 + m2)/m1× √2ππ¦, was used to determine the first initial firing velocity of the steel ball (EV1). As for the horizontal projectile, since the experimenters haven’t change the firing position of the launcher, the firing vertical distance was given to be the same with the initial height (y1), y* = 3.2-cm. Then, the ball’s distance was predicted before a carbon paper and a bond paper was used. These papers were used to mark the landing of the ball. The steel ball was fired and its horizontal distance was measured for five times that averaged x* = 45.86π cm. Later on, the equation no. 7, V1 = x × √2π¦∗, was used to compute the second initial speed of the steel ball to be one of the experimental values (EV2). Lastly, the percent difference |πΈπ1−πΈπ2| was calculated with the formula % ππππ = πΈπ1+πΈπ2 × 100, % diff = 13.0795%. 2 SAMPLE COMPUTATION π πππ’ππππ: πΌπππ‘πππ π ππππ ππ π‘βπ π π‘πππ ππππ (ππΌ ) = ? (πΈπ. 4) πΌπππ‘πππ π ππππ ππ π‘βπ π π‘πππ ππππ (π1 ) = ? (πΈπ. 7) πΊππ£ππ: πππ π ππ π‘βπ π π‘πππ ππππ, π1 = 65.875 g πππ π ππ π‘βπ πππππ’ππ’π, π2 = 141.7 π (πππππ πππ π = 241.7 π) πΌππππππ π ππ βπππβπ‘ (π¦) = 5.8 ππ πΌπππ‘πππ βπππβπ‘ (π¦ ∗) = 3.2 ππ π΄π£πππππ βππππ§πππ‘ππ πππ π‘ππππ(π₯ ∗) = 45.86 ππ πΉππππ’πππ : (π1 + π2 ) ππΌ = √2ππ¦ π1 π1 = π₯ ∗ √ π 2π¦ ∗ ππππ’π‘ππππ : (65.875 + 241.7) √2(9.8)5.8 65.875 = 4.669070209 (10.66208235) = 49.782 ππ/π ππΌ = π1 = 45.86√ 9.8 2(3.2) = 56.7489 ππ/π π΄ππ π€πππ : ππΌ = 49.782 ππ/π ; π1 = 56.7489 ππ/π CONCLUSION A ballistic pendulum is an equipment which is applied in measuring the speed of a ball (or bullet). This apparatus was used for illustrating the principle, Conservation of energy and momentum. The analysts performed the experiment to observe the principle itself and determined the initial speed of the steel ball using the ballistic pendulum. In conclusion, the researchers learned that if there are no external forces acted, the momentum and energy of the ball and pendulum are both conserved. They can determine and calculate the initial velocity of the steel ball by the law of conservation of energy and the law of conservation of momentum. This initial velocity was compared to the data gathered from the initial velocity of the steel ball in horizontal projectile motion. These data were near to each other that resulted to a low percent difference; thus, really proves the two principles (or laws). However, such errors cannot be avoided. These errors are the air resistance coming from the room and the friction of the system which will enable the system to lose some energy.