PATTS COLLEGE OF AERONAUTICS ESCI 322 DYNAMICS OF RIGID BODIES Different types of speed And velocity Engr. Jabes A. Isoli_____ Instructor * Linear Speed – The time rate of motion of a point along its path‚ or the rate at w/c a point is “approaching” or receding form another point in its path. The 100 meter dash ends at the end of the straight-away. * Angular speed – The time rate of turning of a body about axis. Or the
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Ball Drop Lab 2 Name Date Objective to determine the acceleration of gravity for falling objects to prove that this acceleration is the same for all objects regardless of their mass Apparatus objects to drop‚ stopwatch‚ meter stick‚ Pasco motion sensor Procedure Each group will get 1 object record the balls mass Using a meter stick measure a height (distance) that you are going to drop your ball. Making sure that your initial velocity of the ball is 0 m/s‚ drop the ball and measure (using
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understanding on the different concepts regarding Constant and Uniformly Accelerated Motion. Upon finishing the SIM‚ the reader is expected to: • identify the motion of an object in terms of distance or displacement‚ speed or velocity‚ and acceleration UNDESPICABLE MECHANICS CHANICS GUIDE CARD ACTIVITY CARD ENRICHMENT CARD ASSESSMENT CARD REFERENCE CARD UNDESPICABLE MECHANICS GUIDE CARD The Guide card presents the big picture‚ I’ll give you the overview of the lesson
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Motion NCERT Chapter Questions and Answers and other Q & A Q1: An object has moved through a distance. Can it have zero displacement? If yes‚ support your answer with an example. Answer: Yes an object can have zero displacement even though it has moved through a distance. It happens when the object moves back to its original position i.e. final position coincides with the starting position. Example: Suppose an object travels from O to C and then comes back to original position O. Total
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0 DISCUSSIONS 9 6.0 CONCLUSIONS 10 7.0 APPENDIX 11 ABSTRACT Motion of the rocket is simulated using two numerical analysis methods. From the simulation different parameters such as altitude‚ velocity‚ acceleration and range for initial fuel flows were calculated. Two numerical methods‚ Euler’s integration and 4th order Runge-Kutta integration are used for calculating different parameters for the vertically launched rocket. The efficiency and the accuracy
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|9.61 |9.87 |9.76 |9.82 | Analysis 1. | |Minimum |Maximum |Average | |Acceleration(m/sec2) |9.61 |9.87 |9.74 | The position-time graph is a parabola.It has an increasing and positive slope. 3.The velocity vs. time graph is linear. The
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described as equations. Also‚ we calculated the accelerations of every stage (aup‚ adown and ahighest). Then the relationship among aup‚ adown and ahighest was concluded. Finally‚ the acceleration was measured and was proved from data. Introduction If there is a car launched from the bottom of an incline and it goes up until reaching the highest point‚ then it reverses its direction. To ensure the safety under this circumstance‚ the accelerations of every stage need to be measured in order to
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intervals on a diagram; (3) drawing vectors showing displacement‚ velocity‚ and acceleration and their x and y components at different times. (4) using vector equations to represent velocity and acceleration vectors quantitatively. In this activity you will practice representing the motion shown in Figure 1 using vectors and vector equations that represent displacements as well as average velocities and accelerations in the 1/15th of a second time intervals between position measurements. Figure
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Projectile Motion Purpose: An object in a projectile motion move horizontally with no acceleration and vertically with the gravitational acceleration at the same time. This experiment is to investigate projectile motion using experiments‚ equations and comparing the expected and experimental data. Procedure: Case I: Use formulas to find equation of horizontal Range (R) in a projectile motion. Rearrange equation for Rmax‚ and find the angle Adjust the launches angle to angle Launch
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Laboratory III: Forces Problem IV: Normal and Kinetic Frictional Force I John Greavu March 13‚ 2013 Physics 1301W‚ Professor: Evan Frodermann‚ TA: Mark Pepin Abstract The dependence of two-dimensional velocity and position components on time as well as whether or not said components are constant was determined. Video was recorded of a ball being projected laterally and data of its flight were plotted. From analyzing the data and the corresponding graphs that followed‚ it was shown that while the
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