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The Atwood machine was invented in 1784 by, yes Mr. Atwood. Two weights of mass M and m<M are connected by a string over a pulley. The acceleration is

a = \frac{M-m}{M+M}g

Here is a demonstration from MIT, USA:

Homework: check that the experiment measures an acceleration as given by the equation above.

When an object moves in a circular orbit (of radius R), the acceleration has two components, tangential and radial. The angular speed is defined as \omega=d\theta/dt, and angular acceleration defined as \alpha=d^2\theta/dt^2 (\theta is the angle that measures the movement of the position vector); the two components are then generally:

a_{tan} = R\alpha,

a_{rad} = R\omega^2 = \frac{v^2}{R}.

In many cases we work with uniform circular motion, in this case a_{tan}=0.

credit: Prof. Walter Lewin of MIT (course 8.01, Physics I: Classical Mechanics, fall 1999).

Topics covered in this lecture:

Circular Motion – Centrifuges Moving – Reference Frames – Perceived Gravity

George Polya (1887-1985) was a Hungarian mathematician. He is famous for work on mathematics education, and for the 4 steps to solve a problem:

1. understand the problem

2. devise a plan

3. carry out the plan

4. look back

We can use this method to solve physics problems also. Try it! (It is a good idea to make a drawing of the situation in step 1). Single page explaining Polya’s principles:

how-to [PDF]

credit: Prof. Walter Lewin of MIT (course 8.01, Physics I: Classical Mechanics, fall 1999).

Topics covered in this lecture:

Vectors — dot product — cross product — kinematics — projectile motion

(Young and Freedman, chap. 3)

Projectile motion: footballs, humans and pianos – they all (ideally) move in the same way. Try the interactive simulation by following this link. The equation of motion is just

x=x_0+(v_0\cos\alpha)t

y=y_0+(v_0\sin\alpha)t-(1/2)g t^2

[the simulation is from University of Colorado at Boulder].

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