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PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 12
PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 12

3.1-3.2 Circular Motion - York Catholic District School Board
3.1-3.2 Circular Motion - York Catholic District School Board

lectur~4-1 - Dr. Khairul Salleh Basaruddin
lectur~4-1 - Dr. Khairul Salleh Basaruddin

... momentum, denoted as L. This vector has the same direction as v. The linear momentum vector has units of (kg·m)/s or (slug·ft)/s. Linear impulse: The integral F dt is the linear impulse, denoted I. It is a vector quantity measuring the effect of a force during its time interval of action. I acts in ...
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... 13. The figure above represents two carts, with magnets attached, that make up a system. The mass of one cart and magnet is 1 kg and the mass of the other is 5 kg. The carts are initially at rest on a frictionless track. They are released from rest and exert a repulsive force on each other. The tra ...
Momentum and Impulse MC practice problems
Momentum and Impulse MC practice problems

Robot Kinetics – Slide Set 10
Robot Kinetics – Slide Set 10

... Robot Dynamics – Slide Set 10 ...
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2. Laws of Motion

... acceleration of an object of known mass. • State that objects of larger mass require greater forces to cause large acceleration. • Determine the direction of the acceleration on an object. Some students should be able to: • Rearrange and use the equation: force = mass x acceleration. ...
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Motion

Section 3.1.jnt - Lone Star College
Section 3.1.jnt - Lone Star College

Q: Who established the law of universal gravitation? Q: What is a
Q: Who established the law of universal gravitation? Q: What is a

with momentum - Cloudfront.net
with momentum - Cloudfront.net

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Physics 207: Lecture 2 Notes

... Momentum is a Vector (!) quantity x-direction: No net force so Px is conserved.  y-direction: Net force, interaction with the ground so depending on the system (i.e., do you include the Earth?) Py is not conserved (system is block and cart only) ...
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Ch.6 Momentum

... 2 Object Momentum Conservation • momentum before = momentum after • (m1v1)initial + (m2v2)initial = (m1v1)final + (m2v2)final • When can we use this equation? • When net force due to all other objects acting on 1 and 2 is zero. • Or, very soon after collision ends ...
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Physical Science Curriculum 11 2010

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... Block A moves with a velocity of 2 meters per second to the right, as shown in the diagram, and then collides elastically with block B, which is at rest. Block A stops moving, and block B moves to the right after the collision. ...
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... a. Speed- distance an object travels per unit of time. 1. Calculating Speed a. Change over time is called rate b. Speed = distance ÷ time c. SI unit for distance is meter and unit for time is second so speed is measured in meters per second. 2. Motion with Constant Speed a. If you are traveling at a ...
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Momentum and Impulse NOTES PPT

... – Greater time will reduce the chance of dying in a ...
Robot Kinetics * Slide Set 10
Robot Kinetics * Slide Set 10

Linear Kinetics - Weber State University
Linear Kinetics - Weber State University

Reveiw PPT 3_Forces_CM_Momentum_Impulse
Reveiw PPT 3_Forces_CM_Momentum_Impulse

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ME 242 Chapter 13
ME 242 Chapter 13

P3: Forces for Transport
P3: Forces for Transport

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SAMPLE TEST 1: PHYSICS 103

Chapter #7 Giancoli 6th edition Problem Solutions
Chapter #7 Giancoli 6th edition Problem Solutions

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Specific impulse

Specific impulse (usually abbreviated Isp) is a measure of the efficiency of rocket and jet engines. By definition, it is the impulse delivered per unit of propellant consumed, and is dimensionally equivalent to the thrust generated per unit propellant flow rate. If mass (kilogram or slug) is used as the unit of propellant, then specific impulse has units of velocity. If weight (newton or pound) is used instead, then specific impulse has units of time (seconds). The conversion constant between these two versions is the standard gravitational acceleration constant (g0). The higher the specific impulse, the lower the propellant flow rate required for a given thrust, and in the case of a rocket, the less propellant needed for a given delta-v, per the Tsiolkovsky rocket equation.Specific impulse is a useful value to compare engines, much like miles per gallon or liters per 100 kilometers is used for cars. A propulsion method and system with a higher specific impulse is more propellant-efficient. While the unit of seconds can seem confusing to laypeople, it is fairly simple to understand as ""hover-time"": how long a rocket can ""hover"" before running out of fuel, given the weight of that propellant/fuel. Of course, the weight of the rocket has to be taken out of consideration and so does the reduction in fuel weight as it's expended; the basic idea is ""how long can any given amount of x hold itself up"". Obviously that must mean ""...against Earth's gravity"", which means nothing in non-Earth conditions; hence Isp being given in velocity when propellant is measured in mass rather than weight, and the question becomes ""how fast can any given amount of x accelerate itself?""Note that Isp describes efficiency in terms of amount of propellant, and does not include the engine, structure or power source. Higher Isp means less propellant needed to impart a given momentum. Some systems with very high Isp (cf. ion thrusters) may have relatively very heavy/massive power generators, and produce thrust over a long period; thus, while they are ""efficient"" in terms of propellant mass carried, they may actually be quite poor at delivering high thrust as compared to ""less efficient"" engine/propellant designs.Another number that measures the same thing, usually used for air breathing jet engines, is specific fuel consumption. Specific fuel consumption is inversely proportional to specific impulse and the effective exhaust velocity. The actual exhaust velocity is the average speed of the exhaust jet, which includes fuel combustion products, nitrogen, and argon, as it leaves air breathing engine. The effective exhaust velocity is the exhaust velocity that the combusted fuel and atmospheric oxygen only would need to produce the same thrust. The two are identical for an ideal rocket working in vacuum, but are radically different for an air-breathing jet engine that obtains extra thrust by accelerating the non-combustible components of the air. Specific impulse and effective exhaust velocity are proportional.
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