Why Is Average Velocity Calculated Differently in Various Scenarios?

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Discussion Overview

The discussion revolves around the calculation of average velocity in different scenarios, particularly focusing on kinematic equations and the implications of varying velocities. Participants explore the differences in average velocity calculations for a car's journey and a space shuttle's ascent, examining concepts of displacement, speed, and the effects of direction on these calculations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes a scenario involving a car that travels back and forth, questioning the discrepancy between average velocity calculated using displacement versus the average of initial and final velocities.
  • Another participant agrees that the equation (Vfinal + Vinitial)/2 applies only under constant acceleration and suggests that average velocity can still be defined as net displacement over total time.
  • A participant raises a point about the space shuttle's trajectory, noting that while it reaches a high speed, the actual distance traveled is influenced by the angle of ascent, leading to confusion about the relationship between speed and distance.
  • Another participant emphasizes the distinction between velocity (a vector) and speed (a scalar), clarifying that average velocity is based on displacement and can be zero if the starting and ending positions are the same.
  • There is a discussion about the path of the shuttle, with one participant suggesting that the distance traveled along the curved path is different from the vertical height achieved.

Areas of Agreement / Disagreement

Participants express differing views on the application of average velocity calculations, particularly regarding the conditions under which certain equations are valid. There is no consensus on the implications of these calculations in the discussed scenarios.

Contextual Notes

Participants note limitations in understanding related to the definitions of average velocity versus speed, and the impact of direction and path on these calculations. The discussion highlights unresolved aspects of how to accurately represent motion in varying contexts.

Who May Find This Useful

This discussion may be useful for students and educators in physics or related fields, particularly those interested in kinematics and the conceptual differences between velocity and speed.

supernova88
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I'm trying to understand the kinematic equations well enough to explain to someone else, but the analogies I've come up with don't seem to be working well.

1) If a car travels 25 km/h for a certain distance, turns around in the opposite direction, and then turns back on its original path yet again before reaching its destination, then on a distance vs time graph its average velocity is found using the pythagorean theorem for how far the destination is from the origin versus the total time of the trip. This will be far less than 25 km/h. However, according to the equation (Vfinal + Vinitial)/2 = Vaverage, if its initial and final velocities are both 25 km/h in the same direction then the average velocity should be (25 + 25)/2 = 25 km/h. What is the discrepancy between these two versions of the average velocity? I believe the issue is (Vfinal + Vinitial)/2 only applies for cases of constant acceleration, which makes me wonder why we would say there is an average velocity at all if the velocity is constantly changing.

2) A space shuttle reaches orbital velocity of 28,000 km/h in 8.5 minutes (0.1417 h). On a velocity vs time graph this should form a triangle as velocity grows from 0 to 28,000 km/h. The distance should therefore be the area under the curve where the base (time) is 0.1417 h and the height (velocity) is 28,000 km/h. The area, and distance, is therefore 1/2(0.1417 h) (28,000 km/h) = 1983.8 km. However the space shuttle orbits at a height of 360 km give or take. I think the confusion is in the fact the space shuttle doesn't fly straight up but at an angle, so it travels 2,000 km but only as high as 360 km, but I'm not positive on this fact.
 
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supernova88 said:
I believe the issue is (Vfinal + Vinitial)/2 only applies for cases of constant acceleration,

Yes, this is why it doesn't apply to your situation (1).

which makes me wonder why we would say there is an average velocity at all if the velocity is constantly changing.

Imagine measuring and recording the instantaneous velocity (e.g. by looking at a car's speedometer) at frequent regular time intervals, say once per second during a one-hour trip. At the end of the trip, calculate the average of these measurements. (Of course, it's simpler if the trip is back and forth along a straight line; otherwise you have to deal with vector components.) This average will be very nearly equal to the simple ratio (net displacement)/(total elapsed time) which is the usual definition of "average velocity". The shorter the time intervals between measurements, the better the agreement.

2) [...] I think the confusion is in the fact the space shuttle doesn't fly straight up but at an angle, so it travels 2,000 km but only as high as 360 km, but I'm not positive on this fact.

The shuttle's path is curved: it starts out traveling vertically upwards, then curves towards the horizontal, parallel to the Earth's surface. The 2000 km is the distance along this path. (assuming constant magnitude of acceleration of course)
 
Thanks for all the help. I thought I understood where I was confused but I needed some confirmation.
 
It is better to distinguish between velocity (a vector) and speed (a scalar). Strictly speaking, the average velocity over some time interval is the displacement (a vector) divided by the time: ##\frac{\int \vec v.dt}{\int dt}##. In your first example, the return trip reduces the displacement. Once back at the start position, the average velocity for the whole trip is zero.

For the rocket, again, you really mean speed, which is distance traveled along the path divided by time: ##\frac{\int |\vec v|.dt}{\int dt}##.
 

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