Lecture 2: 1D Kinematics - Speed - Velocity - Acceleration

author: Walter H. G. Lewin, Center for Future Civic Media, Massachusetts Institute of Technology, MIT
recorded by: Massachusetts Institute of Technology, MIT
published: Oct. 10, 2008,   recorded: September 1999,   views: 19063
released under terms of: Creative Commons Attribution Non-Commercial Share Alike (CC-BY-NC-SA)

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1. Introduction to 1-Dimensional Motion:

Professor Lewin describes 1D motion of a particle. He talks about average velocity, the importance of "+" and "-" signs, and our free choice of origin.

2. Average Speed vs. Average Velocity:

The two are VERY different. The average velocity can be ZERO, while the average speed is LARGE.

3. Instantaneous Velocity:

Considering the incremental change in position x with time t, we arrive at v=dx/dt. The instantaneous velocity is the derivative of the position with respect to time. Professor Lewin reviews when the velocity is zero, positive and negative; he distinguishes speed from velocity.

4. Measuring the Average Speed of a Bullet:

Professor Lewin shoots a bullet through two wires. The average speed can be calculated from the distance between the wires and the elapsed time. All uncertainties in the measurements are discussed; they have to be taken into account in the final answer.

5. Introducing Average Acceleration:

The average acceleration between time t1 and t2 is the vectorial change in velocity divided by (t2-t1).

6. Instantaneous Acceleration:

The acceleration, dv/dt, is the derivative of the velocity with time. It is the second derivative of the position x with time. Professor Lewin shows how to find the sign of the acceleration from the slope in an x-t plot.

7. Quadratic Equation of Position in Time:

When the position is proportional to the square of the time, the velocity depends linearly on time, and the acceleration is constant.

8. 1D Motion with Constant Acceleration:

Professor Lewin writes down a general quadratic equation for the position as a function of time, and he relates the constants in this equation to the initial conditions at time t=0. The gravitational acceleration is a constant (9.80 m/s^2 in Boston), and it is independent of the mass and shape of a free-falling object, if air drag can be ignored (see Lecture #12). You can use this result to measure g using the free fall time measurements from the falling apples in lecture 1. 9. Strobing an Object in Free Fall: Professor Lewin drops an apple from 3.20 m and takes a polaroid picture of the falling apple which is illuminated by a strobe light. First two light flashes per second, and then ten flashes per second.

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Reviews and comments:

Comment1 Fred, December 14, 2009 at 9:03 p.m.:

awesome!


Comment2 Rahul Bhambure, January 17, 2010 at 7:42 a.m.:

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Comment4 Apostolis, September 10, 2010 at 1:53 a.m.:

Excellent presentation by Dr. Lewin, even a dummy like myself can grip it.
One important observation:
the lecture is easily understood even by a non native english language speaker very well.


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Comment14 asim sajjad, June 14, 2016 at 8:48 p.m.:

Mr,Walter is the best teacher i have ever seen.he delivers lecture in an amazing way.i have learn so many things from him.


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Comment16 Davor form VideoLectures, December 18, 2017 at 10:34 a.m.:

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