JC2 Term 1 Mechanics

Chapter 3: Forces in two dimensions

Chapter 2: Force and motion in one dimension

Chapter 1: Velocity & Acceleration

SUVAT EQUATIONS

v=u+at

S=ut + 1/2 at^2

v^2=u^2+2as

V^2 = u^2 + 2as

Chapter 4: Friction

μ = F/R

W=mg

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The symbol is the coefficient, the F is the friction and R is the normal contact force

Newton's second law

F=ma

Tension

R^2 =x^2 + y^2

Tanθ=Ry/Rx

Weight components down the slope

Figure_04_05_03

DF-R-wcosθ=m.a

Limiting equilibrium

Equilibrium Fx = Fy

Limiting equilibrium

Imagine that you are trying to push a book along a table with your finger. If you apply a very small force, the book will not move. This must mean that the frictional force is equal to the force with which you are pushing the book. If the frictional force were less that the force produced by your finger, the book would slide forward. If it were greater, the book would slide backwards.

If you push the book a bit harder, it would still remain stationary. The frictional force must therefore have increased, or the book would have moved. If you continue to push harder, eventually a point is reached when the frictional force increases no more. When the frictional force is at its maximum possible value, friction is said to be limiting. If friction is limiting, yet the book is still stationary, it is said to be in limiting equilibrium. If you push ever so slightly harder, the book will start to move. If a body is moving, friction will be taking its limiting value.

The frictional force between two objects is not constant, but increases until it reaches a maximum value. When the frictional force is at its maximum, the body in question will either be moving or will be on the verge of moving.

Normal contact force

Air resistance

Components

W=fdcosθ