HW2solutions - Physics 213 HW #2 Solutions Spring 2009...

Info iconThis preview shows pages 1–2. Sign up to view the full content.

View Full Document Right Arrow Icon
Physics 213 HW #2 – Solutions Spring 2009 21.59. [E-Field Lines & Particle Paths] Remember that electric field lines are constructed so that the tangent to the field line at any point gives the direction of the electric field at that point. The electric force is proportional to the electric field, so the force vector (on a positive charge) will point in the same direction as the electric field. Since the acceleration is proportional to the force, the acceleration vector will point along the tangent to the electric field line. Now let’s consider the particle’s trajectory. If we look at the path the particle follows, the velocity vector at a point on the path is tangent to the path at that point. So the shape of the electric field lines tell us about the acceleration, and the shape of the particle’s path tells us about the velocity. (a) In Fig.21.29a, the field lines are straight lines so the force is always in a straight line and velocity and acceleration are always in the same direction. The particle moves in a straight line along a field line, with increasing speed. (b) In Fig.21.29b, the field lines are curved. Suppose the charged particle followed the path of one of these curved field lines. Remember that, for the particle to follow a curved path, its acceleration must have a component perpendicular to the path. This is not possible if the particle is following a field line, since the electric field (and, hence, the acceleration) must be tangent to the field line. So the path the particle follows must be different. As the particle moves its velocity and acceleration are not in the same direction and the trajectory does not follow a field line. In conclusion, two-dimensional motion the velocity is always tangent to the trajectory but the velocity is not always in the direction of the net force on the particle. 21.61. [Infinite Line Charge E-Field Lines] We use symmetry to deduce the nature of the field lines. (a) The only distinguishable direction is toward the line or away from the line, so the electric field lines are perpendicular to the line of charge, as shown in the figures to the right. (c) From the figures above, we see that the main difference between the electric field from a point charge and the electric field of a charged line is that the field lines from a point charge spread out in all three dimensions, while the field lines from a line of charge spread out in only two dimensions—the dimensions perpendicular to the line. The magnitude of the electric field is inversely proportional to the spacing of the field lines, so spreading out in fewer dimensions means the field falls off more slowly. To see how this spacing between field lines changes with r , the distance from the line, imagine that the line of charge is surrounded by a cylinder of radius r centered on the charged line. Since all of the spreading is done in the directions perpendicular to the line, it is sufficient to look at the field in a plane perpendicular to the line. This is shown on the figure to the right. One sees that, on this plane, the line of charge appears as a point, the cylinder appears as a circle, and the field lines are radial lines.
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
Image of page 2
This is the end of the preview. Sign up to access the rest of the document.

This note was uploaded on 04/14/2009 for the course PHYS 2213 taught by Professor Perelstein,m during the Spring '07 term at Cornell University (Engineering School).

Page1 / 5

HW2solutions - Physics 213 HW #2 Solutions Spring 2009...

This preview shows document pages 1 - 2. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online