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An electron moving along the \(x\) axis has a position given by \(x=16 t e^{-t} \mathrm{~m}\), where \(t\) is in seconds. How far is the electron from the origin when it momentarily stops?

Short Answer

Expert verified
The electron is \( \frac{16}{e} \) meters from the origin when it momentarily stops.

Step by step solution

01

Find the Expression for Velocity

The velocity of the electron is the derivative of its position with respect to time. Begin by finding the derivative of the given position function, which is:\[ x(t) = 16t e^{-t} \]Using the product rule (\(uv' + vu'\)), where \(u = 16t\) and \(v = e^{-t}\), compute each derivative:- \(u' = 16\)- \(v' = -e^{-t}\)So the derivative, velocity \(v(t)\) is:\[ v(t) = 16 \cdot e^{-t} + (-e^{-t}) \cdot 16t \]Simplifying gives:\[ v(t) = 16e^{-t} - 16t e^{-t} = 16(1-t) e^{-t} \]
02

Set Velocity to Zero to Find Critical Points

The electron momentarily stops when its velocity is zero. Setting the expression from Step 1 to zero, we have:\[ 16(1-t) e^{-t} = 0 \]Since \(e^{-t} eq 0\), we divide by this term (it will never be zero), and solve the simplified equation:\[ 16(1-t) = 0 \]This gives:\[ 1-t = 0 \]\[ t = 1 \]
03

Calculate Position at When Velocity is Zero

Substitute the critical time \(t = 1\) back into the original position function to find the position of the electron:\[ x = 16 \cdot 1 \cdot e^{-1} = \frac{16}{e} \]This is the distance from the origin when the electron stops.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Derivatives in Physics
In physics, one of the most important concepts is the derivative, which helps us understand how things change over time. The derivative can tell us the rate at which a function is changing. For example, if we have the position function of an object, like an electron in motion, the derivative of this position function with respect to time will give us the velocity. The position function in our original example is ‎\( x(t) = 16t e^{-t} \)‎, a product of two functions of \(t\).
To find the electron's velocity, we differentiate its position with respect to time. This results in the function describing how fast the electron moves at any given moment. Derivatives play a key role in physics because they allow us to determine the instantaneous speed of an object or how an object's speed changes over time.
For students, mastering the derivative concept will greatly aid in understanding motion, especially how velocity and acceleration relate to an object's position.
Product Rule in Calculus
When dealing with problems involving derivatives, the product rule is a crucial technique, especially for functions that are products of two or more functions.
The product rule is stated as follows: if you have two functions \( u \) and \( v \), the derivative of their product \( uv \) is \( uv' + vu' \). In other words, you differentiate each function separately and then combine them appropriately.
In our example, we've identified \( u = 16t \) and \( v = e^{-t} \). Using the product rule, we find:
  • The derivative of \( u \), \( u' = 16 \).
  • The derivative of \( v \), \( v' = -e^{-t} \).
Therefore, the derivative of \( x(t) = 16t e^{-t} \) is \( 16e^{-t} - 16t e^{-t} = 16(1-t) e^{-t} \).
This technique allows us to find derivatives of more complex functions systematically, aiding in solving various physics and engineering problems.
Critical Points in Motion
In motion analysis, critical points are moments when an object's velocity is zero, indicating that the object has momentarily stopped or changed its direction. Finding these points is essential in understanding the motion characteristics of an object.
In our context, we discovered the point in time at which the electron stops by setting its velocity function to zero: \( 16(1-t)e^{-t} = 0 \). After simplifying, we conclude \( t = 1 \) because the exponential function \( e^{-t} \) never equals zero.
At \( t = 1 \), the velocity is zero, meaning the electron is momentarily at rest. Substituting back into the position function gives us the location \( \frac{16}{e} \) meters from the origin. Critical points help us pinpoint when and where certain events take place in motion.

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Most popular questions from this chapter

The sport with the fastest moving ball is jai alai, where measured speeds have reached \(303 \mathrm{~km} / \mathrm{h}\). If a professional jai alai player faces a ball at that speed and involuntarily blinks, he blacks out the scene for \(100 \mathrm{~ms}\). How far does the ball move during the blackout?

The wings on a stonefly do not flap, and thus the insect cannot fly. However, when the insect is on a water surface, it can sail across the surface by lifting its wings into a breeze. Suppose that you time stoneflies as they move at constant speed along a straight path of a certain length. On average, the trips each take \(7.1 \mathrm{~s}\) with the wings set as sails and \(25.0 \mathrm{~s}\) with the wings tucked in. (a) What is the ratio of the sailing speed \(v_{s}\) to the nonsailing speed \(v_{n s} ?(\mathrm{~b})\) In terms of \(v_{s}\), what is the difference in the times the insects take to travel the first \(2.0 \mathrm{~m}\) along the path with and without sailing?

A stone is thrown vertically upward. On its way up it passes point \(A\) with speed \(v\), and point \(B, 3.00 \mathrm{~m}\) higher than \(A\), with speed \(\frac{1}{2} v .\) Calculate (a) the speed \(v\) and (b) the maximum height reached by the stone above point \(B\).

The head of a rattlesnake can accelerate at \(50 \mathrm{~m} / \mathrm{s}^{2}\) in striking a victim. If a car could do as well, how long would it take to reach a speed of \(100 \mathrm{~km} / \mathrm{h}\) from rest?

A train started from rest and moved with constant acceleration. At one time it was traveling \(30 \mathrm{~m} / \mathrm{s}\), and \(160 \mathrm{~m}\) farther on it was traveling \(50 \mathrm{~m} / \mathrm{s}\). Calculate (a) the acceleration, (b) the time required to travel the \(160 \mathrm{~m}\) mentioned, \((\mathrm{c})\) the time required to attain the speed of \(30 \mathrm{~m} / \mathrm{s}\), and \((\mathrm{d})\) the distance moved from rest to the time the train had a speed of \(30 \mathrm{~m} / \mathrm{s}\). (e) Graph \(x\) versus \(t\) and \(v\) versus \(t\) for the train, from rest.

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