banner



How Do You Know Where To Draw Electric Field (E) At Point P

Electric Field Lines

In the previous department of Lesson 4, the vector nature of the electric field strength was discussed. The magnitude or strength of an electric field in the infinite surrounding a source charge is related directly to the quantity of charge on the source charge and inversely to the distance from the source accuse. The direction of the electric field is always directed in the direction that a positive test charge would be pushed or pulled if placed in the space surrounding the source charge. Since electric field is a vector quantity, it tin be represented past a vector pointer. For any given location, the arrows point in the direction of the electric field and their length is proportional to the strength of the electric field at that location. Such vector arrows are shown in the diagram below. Annotation that the lengths of the arrows are longer when closer to the source charge and shorter when farther from the source charge.

A more useful means of visually representing the vector nature of an electric field is through the use of electric field lines of force. Rather than draw countless vector arrows in the space surrounding a source charge, it is perhaps more useful to draw a pattern of several lines that extend betwixt infinity and the source charge. These pattern of lines, sometimes referred to as electrical field lines , bespeak in the direction that a positive test charge would accelerate if placed upon the line. As such, the lines are directed away from positively charged source charges and toward negatively charged source charges. To communicate information almost the direction of the field, each line must include an arrowhead that points in the appropriate direction. An electric field line pattern could include an infinite number of lines. Because drawing such large quantities of lines tends to decrease the readability of the patterns, the number of lines is usually limited. The presence of a few lines around a accuse is typically sufficient to convey the nature of the electric field in the space surrounding the lines.


Rules for Drawing Electrical Field Patterns

There are a variety of conventions and rules to cartoon such patterns of electric field lines. The conventions are only established in order that electric field line patterns communicate the greatest amount of information about the nature of the electric field surrounding a charged object. Ane mutual convention is to surroundings more charged objects by more than lines. Objects with greater charge create stronger electric fields. By surrounding a highly charged object with more than lines, one can communicate the forcefulness of an electrical field in the space surrounding a charged object by the line density. This convention is depicted in the diagram beneath.

Non merely does the density of lines surrounding any given object reveal information about the quantity of accuse on the source charge, the density of lines at a specific location in space reveals information about the strength of the field at that location. Consider the object shown at the right. Two unlike circular cross-sections are drawn at different distances from the source charge. These cross-sections represent regions of infinite closer to and farther from the source charge. The field lines are closer together in the regions of space closest to the charge; and they are spread further apart in the regions of space furthest from the charge. Based on the convention concerning line density, 1 would reason that the electric field is greatest at locations closest to the surface of the charge and least at locations farther from the surface of the accuse. Line density in an electric field line pattern reveals information about the forcefulness or magnitude of an electric field.

A second rule for drawing electric field lines involves drawing the lines of force perpendicular to the surfaces of objects at the locations where the lines connect to object's surfaces. At the surface of both symmetrically shaped and irregularly shaped objects, there is never a component of electric force that is directed parallel to the surface. The electric force, and thus the electrical field, is always directed perpendicular to the surface of an object. If there were e'er whatever component of force parallel to the surface, then any backlog accuse residing upon the surface of a source charge would begin to accelerate. This would pb to the occurrence of an electric current within the object; this is never observed in static electricity. In one case a line of force leaves the surface of an object, it will ofttimes alter its direction. This occurs when drawing electric field lines for configurations of 2 or more charges as discussed in the section beneath.

A final rule for cartoon electrical field lines involves the intersection of lines. Electric field lines should never cross. This is particularly important (and tempting to break) when cartoon electric field lines for situations involving a configuration of charges (equally in the section below). If electrical field lines were ever immune to cross each other at a given location, and then y'all might be able to imagine the results. Electric field lines reveal information about the direction (and the strength) of an electric field within a region of space. If the lines cantankerous each other at a given location, then there must be 2 distinctly different values of electric field with their own private direction at that given location. This could never be the instance. Every unmarried location in infinite has its own electric field strength and direction associated with information technology. Consequently, the lines representing the field cannot cross each other at whatever given location in space.


Electrical Field Lines for Configurations of Two or More Charges

In the examples above, we've seen electrical field lines for the infinite surrounding single point charges. But what if a region of space contains more than than ane point accuse? How can the electric field in the space surrounding a configuration of 2 or more charges exist described past electric field lines? To reply this question, we volition first return to our original method of drawing electrical field vectors.

Suppose that there are two positive charges - charge A (QA) and charge B (QB) - in a given region of space. Each charge creates its ain electrical field. At whatsoever given location surrounding the charges, the strength of the electric field tin be calculated using the expression kQ/dtwo. Since at that place are two charges, the kQ/d2 calculation would have to be performed twice at each location - once with kQA/dA two and once with kQB/dB ii (dA is the distance from that location to the eye of charge A and dB is the altitude from that location to the center of accuse B). The results of these calculations are illustrated in the diagram below with electric field vectors (EA and EB) drawn at a variety of locations. The force of the field is represented by the length of the pointer and the direction of the field is represented by the direction of the pointer.

Since electric field is a vector, the usual operations that employ to vectors can be applied to electrical field. That is, they can be added in head-to-tail fashion to determine the resultant or net electric field vector at each location. This is shown in the diagram below.

The diagram above shows that the magnitude and direction of the electric field at each location is but the vector sum of the electric field vectors for each private charge. If more locations are selected and the process of cartoon EA, EastwardB and Eastnet is repeated, then the electrical field force and direction at a multitude of locations will be known. (This is non done since it is a highly time intensive chore.) Ultimately, the electrical field lines surrounding the configuration of our two charges would begin to sally. For the limited number of points selected in this location, the beginnings of the electric field line pattern can exist seen. This is depicted in the diagram below. Note that for each location, the electric field vectors point tangent to the direction of the electric field lines at whatsoever given point.

The construction of electric field lines in this way is a deadening and cumbersome job. The utilize of a field plotting figurer software program or a lab procedure produces similar results in less time (and with more phun). Whatever the method used to make up one's mind the electric field line patterns for a configuration of charges, the general thought is that the pattern is the resultant of the patterns for the individual charges inside the configuration. The electric field line patterns for other charge configurations are shown in the diagrams below.

In each of the above diagrams, the private source charges in the configuration possess the same amount of charge. Having an identical quantity of accuse, each source charge has an equal ability to alter the space surrounding it. Subsequently, the pattern is symmetrical in nature and the number of lines emanating from a source charge or extending towards a source accuse is the same. This reinforces a principle discussed earlier that stated that the density of lines surrounding whatever given source accuse is proportional to the quantity of charge on that source charge. If the quantity of accuse on a source charge is non identical, the pattern will take on an asymmetric nature, as one of the source charges volition have a greater ability to alter the electrical nature of the surrounding infinite. This is depicted in the electric field line patterns below.

Later on plotting the electrical field line patterns for a variety of charge configurations, the general patterns for other configurations can exist predicted. At that place are a number of principles that volition assist in such predictions. These principles are described (or re-described) in the list beneath.

  • Electric field lines always extend from a positively charged object to a negatively charged object, from a positively charged object to infinity, or from infinity to a negatively charged object.
  • Electric field lines never cross each other.
  • Electrical field lines are nearly dense around objects with the greatest amount of charge.
  • At locations where electric field lines meet the surface of an object, the lines are perpendicular to the surface.

Electric Field Lines as an Invisible Reality

It has been emphasized in Lesson four that the concept of an electric field arose as scientists attempted to explain the activity-at-a-distance that occurs between charged objects. The concept of the electric field was get-go introduced by 19th century physicist Michael Faraday. It was Faraday's perception that the pattern of lines characterizing the electric field represents an invisible reality. Rather than thinking in terms of one charge affecting another accuse, Faraday used the concept of a field to propose that a charged object (or a massive object in the case of a gravitational field) affects the infinite that surrounds information technology. As another object enters that infinite, information technology becomes affected by the field established in that space. Viewed in this manner, a charge is seen to interact with an electric field as opposed to with another charge. To Faraday, the secret to understanding activeness-at-a-altitude is to understand the power of charge-field-charge. A charged object sends its electric field into space, reaching from the "puller to the pullee." Each charge or configuration of charges creates an intricate web of influence in the space surrounding information technology. While the lines are invisible, the result is ever so existent. And then equally you practice the exercise of constructing electric field lines around charges or configuration of charges, you are doing more than merely drawing curvy lines. Rather, you are describing the electrified spider web of infinite that will draw and repel other charges that enter it.

We Would Similar to Advise ...

Sometimes information technology isn't enough to merely read about it. Y'all take to interact with it! And that's exactly what you do when you use one of The Physics Classroom's Interactives. Nosotros would similar to suggest that yous combine the reading of this page with the apply of our Put the Charge in the Goal Interactive and/or our Electric Field Lines Interactive. Both Interactives can be constitute in the Physics Interactives section of our website. Both Interactives provide engaging environments for exploring electric field lines.

Bank check Your Agreement

Employ your understanding to answer the following questions. When finished, click the push to view the answers.

ane. Several electric field line patterns are shown in the diagrams below. Which of these patterns are wrong? _________ Explain what is wrong with all wrong diagrams.

ii. Erin Agin drew the following electric field lines for a configuration of 2 charges. What did Erin do wrong? Explain.

3. Consider the electric field lines shown in the diagram below. From the diagram, it is credible that object A is ____ and object B is ____.

a. +, +

b. -, -

c. +, -

d. -, +

e. insufficient info

iv. Consider the electrical field lines drawn at the right for a configuration of two charges. Several locations are labeled on the diagram. Rank these locations in order of the electric field strength - from smallest to largest.

5. Use your agreement of electric field lines to identify the charges on the objects in the following configurations.

6. Find the electric field lines below for diverse configurations. Rank the objects according to which has the greatest magnitude of electric charge, first with the smallest charge.

Source: https://www.physicsclassroom.com/class/estatics/Lesson-4/Electric-Field-Lines

Posted by: belltrainge.blogspot.com

0 Response to "How Do You Know Where To Draw Electric Field (E) At Point P"

Post a Comment

Iklan Atas Artikel

Iklan Tengah Artikel 1

Iklan Tengah Artikel 2

Iklan Bawah Artikel