Changing the direction of the acceleration Vector

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Homework Help Overview

The discussion revolves around the behavior of electric fields and forces acting on charged particles, specifically focusing on two point charges and their effects on an electron placed in the electric field created by these charges. The original poster describes a scenario involving two charges, one negative and one positive, and the resulting electric field at a specific point.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to understand why the acceleration vector of an electron appears to point in the opposite direction to the electric field. Some participants explore the relationship between charge, electric field, and force, questioning how to interpret the signs in the equations involved.

Discussion Status

Participants are actively engaging with the concepts, with some providing insights into the relationship between electric fields and forces on charged particles. There is a recognition of the role of charge polarity in determining the direction of acceleration, but no consensus has been reached on alternative methods to switch the direction of the acceleration vector without altering the equations directly.

Contextual Notes

Participants are discussing the implications of charge signs and the resulting forces, with an emphasis on understanding the underlying physics rather than deriving a specific solution. There is an acknowledgment of the complexity involved in interpreting the force experienced by different types of charges in an electric field.

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Homework Statement


2 point charges. q1 is -25 microC and q2 is 50 microC are separated by a distance of .1m where q1 is on a line that connects q1 to q2 and q1 is to the left of q2. point p is .02 m to the right of q1 and .8m to the left of q2.


Homework Equations



E = F/q

E(e) = Force on electron due to Electric Field

The Attempt at a Solution



okay, so the electric field at point p due to these 2 point charges is -6.3 E 8 N/C dot i.

if we put an electron at point p, the electron will feel an acceleration.

the electric field points to the left at point p. yet, the electron feels an acceleration vector pointing to the right. How do I switch the direction of the acceleration vector without multiplying a negative to the equation E(-e) = m(acc) where E = -6.3 E 8 N/C dot i ?
 
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so? anybody with any ideas?
 
Your Force equation is the product of the charge scalar and the E-field. Your e-Field at p is -x. But there is a - carried with the e. This reverses the acceleration that the charge will experience.
 
there's got to be another way to switch the direction without multiplying by the negative scalar. If you look inside the Force equation...

f = q q k / r squared dot unit vector r. however, I'm not sure if the positive test charge feels a negative or positive force from the source.
 
Positive test charge experiences positive force (repulsive force) outward from the point charge. The r vector of force is negative directed at that point as a result of the negative position from the net outward from the dominating positive. As a negative the electron however wants to accelerate opposite, i.e. toward the positive point, against the positive gradient, but of course only there and not beyond.
 

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