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Midterm Exam -- Review Problems 1. A 1,000 kg car starts from rest
Midterm Exam -- Review Problems 1. A 1,000 kg car starts from rest

... a. What is the final velocity of the two masses? [Conservation of Momentum] b. What is the final kinetic energy after the collision? [definition of KE] c. *How much kinetic energy is lost in this collision? [definition of change in KE] 5. *[Continuation from #4] Assume the surface to the right of ma ...
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Chapter 19 Outline The First Law of Thermodynamics - Help-A-Bull

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... and each speck of dust is one of our “particles.” On the one hand, if we focus in, we see that each speck is naturally at a different location, has a different mass, and is moving with a different velocity. Yet, if we zoom out, we see a single cloud that behaves somewhat cohesively. If we watch the ...
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... 7) An object following a straight-line path at constant speed A) has zero acceleration. B) has a net force acting upon it in the direction of motion. C) must be moving in a vacuum or in the absence of air drag. D) has no forces acting on it. E) none of these. 8) A skydiver's terminal velocity will ...
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... Its motion is steady and NON – TURBULENT A fluid's motion can be said to be STREAMLINE, or LAMINAR. The path itself is called the streamline. By Laminar, we mean that every particle moves exactly along the smooth path as every particle that follows it. If the fluid DOES NOT have Laminar Flow it has ...
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... function for all problems. So the square root of 25 would be shown as [25]. V2 = [2 X (KE)/m] v = [(2 X 250000 J)/800kg] = [(2 X 250000 N*m)/800 kg] = [(2 X 250000 kg*m2/sec2)/800 kg] = [(500,000 k*m2/sec2)/800 kg] = [625 m2/sec2] = 25 m/sec ...
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K = 1 2 mv W = Fds ︷︸︸︷ = Fd ΑK = K −Ki =W
K = 1 2 mv W = Fds ︷︸︸︷ = Fd ΑK = K −Ki =W

... m1 = 0.5 kg, the speed of the hammer head when it strikes the nail is v1 = 200 m/s. The head then bounces back with a speed of v2 = 100 m/s (opposite direction). The nails mass is m2 = 5g. If the frictional force between the nail and the wood is Ff = 104N, how far will the nail go into the wood? Ste ...
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Momentum Problems (From Merrill Principles and Problems with

... 22. A ball of mass 3 kg, moving a 2 m/s eastward, strikes a 1 kg ball moving westward at 4 m/s. a. If the balls stick together, what is their combined speed and direction after the collision? b. If the balls rebound, with the 3 kg ball moving westward at 1 m/s after the collision, what is the speed ...
AP_Physics_B_-_Fluid_Dynamics
AP_Physics_B_-_Fluid_Dynamics

... A fluid's motion can be said to be STREAMLINE, or LAMINAR. The path itself is called the streamline. By Laminar, we mean that every particle moves exactly along the smooth path as every particle that follows it. If the fluid DOES NOT have Laminar Flow it has TURBULENT FLOW in which the paths are irr ...
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Center of mass



In physics, the center of mass of a distribution of mass in space is the unique point where the weighted relative position of the distributed mass sums to zero or the point where if a force is applied causes it to move in direction of force without rotation. The distribution of mass is balanced around the center of mass and the average of the weighted position coordinates of the distributed mass defines its coordinates. Calculations in mechanics are often simplified when formulated with respect to the center of mass.In the case of a single rigid body, the center of mass is fixed in relation to the body, and if the body has uniform density, it will be located at the centroid. The center of mass may be located outside the physical body, as is sometimes the case for hollow or open-shaped objects, such as a horseshoe. In the case of a distribution of separate bodies, such as the planets of the Solar System, the center of mass may not correspond to the position of any individual member of the system.The center of mass is a useful reference point for calculations in mechanics that involve masses distributed in space, such as the linear and angular momentum of planetary bodies and rigid body dynamics. In orbital mechanics, the equations of motion of planets are formulated as point masses located at the centers of mass. The center of mass frame is an inertial frame in which the center of mass of a system is at rest with respect to the origin of the coordinate system.
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