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Force Problems #3
Force Problems #3

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Ch. 8. Energy

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Ch.2 Linear Motion

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Downlaod File

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Forces and Motion Review Sheeteoct answers

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Examples and problems to the system of particles

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9 Systems of Particles

... Consider the total kinetic energy K  2 mi vi i of a system of particles. This can be rewritten as K = Kcm + Kint, where the first term is the kinetic energy of the center of mass and the second is the kinetic energy relative to the center of mass. ...
IB Mechanics objectives
IB Mechanics objectives

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EXAM 1 – 100 points

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Chapter 09 - Center of Mass and Linear Momentum

... the center of mass comS for disk S is at the center of S, at x =-R. Similarly, the center of mass comC for composite plate C is at the center of C, at the origin. Assume that mass mS of disk S is concentrated in a particle at xS =-R, and mass mP is concentrated in a ...
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Skills Worksheet

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Solved Problems and Questions on fluid properties

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... Vectors 2: Acceleration. • Acceleration is the change in Velocity during some small time interval. Notice that either speed or direction, or both, may change. • For example, falling objects are accelerated by gravitational attraction, g. In English units, the speed of falling objects increases by a ...
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ThePhysicsOfSkydiving - Aponte and Shluger

... gravity pulling down on any object that has mass. If gravity is the only force acting on an object, then we find the object will accelerate at a rate of 9.8m/s2 down toward the center of the Earth. Gravity acts on all bodies in the universe, and each bodies' gravitational effects are related. The bo ...
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... The larger, flatter object will create more air resistance. The flatness of the object will catch more air than the less flat object. Choose the term from the word list that best completes each statement. Write the term in the blank at the left of each statement. action gravity mass ...
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3 - CSUN.edu

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The Top 5- Vectors

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graphs and equations of motion

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C - Energi Masa Depan Weblog | Just another WordPress.com weblog

Unit G484: The Newtonian World
Unit G484: The Newtonian World

Lecture 16: Centripetal Acceleration, ac = v 2/r
Lecture 16: Centripetal Acceleration, ac = v 2/r

... then we find g = 9.8m/s2 . Note also that Newton’s third law applies here, so the force on mass m1 due to mass m2 is equal and opposite to the force on m2 due to m1 . Gravitational potential energy We have so far said that the change in gravitational potential energy near the surface of earth is ∆P ...
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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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