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Smooth Pulley With 1 Load With 2 Loads Vector Stationary: http://www.one-school.net/notes.html T1 = T2 T1 = mg Finding Acceleration: (If m2 > m1) Finding Tension: (If m2 > m1) Vector Addition (Perpendicular Vector) Vector Resolution Magnitude = Direction = 8 ONE-SCHOOL.NET Moving with uniform speed: Accelerating: m2g – m1g = (m1+ m2)a T1 = T2 T1 – m1g = ma m2g – T2 = ma 2 2 x + y −1 | y | tan | x | | x| = | p|sinθ | y | = | p |cosθ T1 = mg T1 – mg = ma
Inclined Plane Forces In Equilibrium Work Done T3= mg T θ = mg 2 sin T cosθ = T 2 1 1 tanθ = T mg W = Fxcosθ When the force and motion are in the same direction. W = Fs http://www.one-school.net/notes.html 9 ONE-SCHOOL.NET Component parallel to the plane = mgsinθ Component perpendicular to the plane = mgcosθ T3= mg T cosθ = T cosα 2 1 T sinθ + T sinα = mg 2 1 W = Work Done (J or Nm) F = Force (N or kgms -2 ) x = displacement (m) θ = angle between the force and the direction of motion ( o ) W = Work Done (J or Nm) F = Force (N or kgms -2 ) s = displacement (m)
Page 1 and 2: Relative Deviation Prefixes Units f
Page 3 and 4: Ticker Tape Finding Velocity: Findi
Page 5 and 6: Newton’s Second Law mv − mu Fα
Page 7: http://www.one-school.net/notes.htm
Page 11 and 12: Density Pressure F P = A http://www
Page 13 and 14: Pascal’s Principle Archimedes Pri
Page 15 and 16: Charles’s Law (Requirement: Press
Page 17: Astronomical Telescope Magnificatio

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