Electron traveling parallel to a Uniform Electric Field

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SUMMARY

An electron traveling parallel to a uniform electric field of magnitude 1.18E4 N/C with an initial speed of 2.0E7 m/s will experience a force calculated using F=qE, resulting in a force of 2.88E-15 N. The acceleration is determined to be 3.16E15 m/s². The distance traveled before stopping can be calculated using the conservation of energy approach, leading to the formula Δx = -mv²/(2eE), which simplifies the process compared to kinematic equations. The correct application of these principles is crucial for accurate results in physics problems involving electric fields.

PREREQUISITES
  • Understanding of electric fields and forces (E=F/q)
  • Knowledge of kinematics and constant acceleration equations
  • Familiarity with conservation of energy principles
  • Basic understanding of electron properties (charge and mass)
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  • Study the conservation of energy in electric fields
  • Learn about the relationship between electric field strength and potential difference
  • Explore kinematic equations for uniformly accelerated motion
  • Investigate the properties and behavior of charged particles in electric fields
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Students and educators in physics, particularly those focusing on electromagnetism and kinematics, as well as anyone solving problems related to charged particles in electric fields.

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Homework Statement



An electron with speed 2.0E7 m/s is traveling parallel to a uniform electric field of magnitude 1.18E4 N/C. How far will the electron travel before it stops? How much time will elapse before it returns to its starting point

q = 1.60E-19 C
mass of electron = 9.11E-31 kg
velocity (initial) = 2.10E7 m/s
velocity(final) = 0 (zero)

Homework Equations


Electric Field
E=F/q --> F=qE

Acceleration / Force equation
a=F/m

Constant Acceleration
v(final)^2=v(initial)^2 +2a*(delta x) --> delta x = (v(final)^2 - v(initial)^2) / 2a


The Attempt at a Solution



F=qE = (1.60E-19 C)(1.8E4 N/C) = 2.88E-15N

a=F/m = (2.88E-15N) / (9.11E-31 kg) = 3.16E15 m/s^2

delta x = (v(final)^2 - v(initial)^2) / 2a
delta x = (0 - 2.10E7 m/s) / 2*(3.16E15 m/s^2)
delta x = -6.97785E-2 m <--- ACCORDING TO MASTERING PHYSICS THIS ANSWER IS WRONG!

with the 2nd part of the question... I was going to use the equation
delta x = 1/2[v(initial) + v(final)]*t
but since my delta x is wrong, i haven't quite started this part...

Any and all help will be appreciated! Thank you in advance!
 
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Welcome to PF,

It looks like you might have slipped up on your arithmetic. The given electric field is 1.18e4 N/C, but you have used 1.8e4 N/C.

By the way, the first part of this question is much easier to solve using conservation of energy. For a uniform electric field, the potential difference between two points is just the electric field strength multiplied by the distance between the two points (V = E*Δx). And the potential energy change for the electron is just the electron charge multiplied by the potential difference. Finally, since the electric force is a conservative force, all of the initial kinetic energy of the electron is converted into electric potential energy (as the electric force does negative work on it to slow it). So you just equate the kinetic and potential energies and solve for Δx.

You'll end up with:

-e*V = (1/2)mv2

where e = 1.60e-19 C is the elementary charge, the smallest unit of charge found in nature (e is the charge of a proton, and -e is the charge of an electron).

-2eEΔx = mv2

Δx = -mv2/(2eE)

Notice that this is just the same formula as the one you obtained using kinematics, since a = F/m = eE/m. However, with this method you arrive at it more quickly. Also, written in this way, it allows you to just plug in all of the given quantities without having to take the intermediate step of computing a.
 
Last edited:
Hmmm... Hahahaha! One digit causing so much trouble. Thank you so much. Your help is much appreciated...
 

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