What is the average of fall distances

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Homework Help Overview

The discussion revolves around a physics problem related to the average distance a rock falls when dropped from a height, with a focus on the mathematical interpretation of distance and time averages in the context of kinematics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore different methods to calculate the average distance fallen, including integrals and the use of velocity equations. Questions arise regarding the notation and the interpretation of variables, particularly the distinction between position and probability in the context of taking measurements at random intervals.

Discussion Status

The discussion is active, with participants sharing their interpretations and approaches. Some express confusion over the notation and the setup of the problem, while others reflect on their own thought processes in tackling the problem. There is no explicit consensus, but various lines of reasoning are being explored.

Contextual Notes

Participants note the potential ambiguity in the problem's wording and the mathematical definitions involved. There is a mention of integrating over time and the implications of different interpretations of the variables used.

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[no template, as this post was moved from here from the Quantum Mechanics forum]

In griffiths 2nd quantum mechnics,

problem : Suppose I drop a rock off a cliff of height h. As if falls, I snap a million photographs, at random intervals. On each picture I measure the distance the rock has fallen.

Question : What is the average of all these distances? That is to say, what is the time average of the distance traveled?

I know p(x) is 1/2(hX)^(1/2) and can solve the problem like : Integral(from 0 to h)x dx/2(hX)^(1/2)

other method is : Integral(from 0 to T) x dt/T

but I don't know how it's possible. that means p(t) = 1/T .. but T is constant{ (2h/g)^1/2}

and I don't know meaning of dt/T
 
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Here's how I would do that- the constant acceleration due to gravity is -g. The velocity, at time t isv(t)= -gt+ v0. Since the rock was "dropped", rather than thrown up or down, v0= 0 and v(t)= -gt. Then the distance traveled in t seconds is s(t)= -(g/2)t^2+ h. The rock will hit the bottom when s(t)= -(g/2)t^2+ h= 0 so when t= \sqrt{2h/g}. The average of a function, f(t), for t between a and b, is \int f(t)dt/(b- a) so the average height, for t between 0 and \sqrt{2h/g} is \frac{\int_0^{\sqrt{2h/g}}( -(g/2)t^2+ h) dt}{\sqrt{2h/g}}
 
I don't understand your notation - I think you mix different things here. p(t) in the first approach looks like the position, while in the second approach it seems to be a probability to take a picture at a specific time. But then the integral should have the position as function of time, not x.
 
I think the problem and his approach was worded so strangely. I had to just close the book and think about it by myself, and figure out how I'd define each piece of the problem mathematically. Then how I could manipulate each piece in order to integrate it. Turned out it was pretty much identical.

Sorry I necro'd this thread. I just had to see if anyone else struggled with this example. Then I wanted to say how I approached the problem so anyone else in the future can maybe try the same type of thing if they were also confused.
 

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