R Circuit: Difference between revisions

From Physics Book
Jump to navigation Jump to search
No edit summary
 
(40 intermediate revisions by 2 users not shown)
Line 1: Line 1:
Page claimed by Trevor Craport
Claimed by Matthew Munns - Fall 2017
Short Description of Topic


==The Main Idea==
Resistors may exist in a circuit and resist electric charge. The resistance of a resistor depends on the properties of the material and the area of the resistor. These two attributes will be investigated later in the page.


State, in your own words, the main idea for this topic
Resistors may be ohmic or non-ohmic. An ohmic resistor has a conductivity that is nearly constant, while a non-ohmic resistor will vary depending on the conditions. This page will focus on ohmic resistors in a complex circuit.
Electric Field of Capacitor


===A Mathematical Model===
The following is an image of an ohmic resistor like the resistor used in lab:
[[File:ResistorResize.jpg]]
==History==  
Georg Simon Ohm, born in 1789, discovered Ohm's law. This law relates the current, voltage, and resistance across a resistor. His law was widely accepted by 1850. Ohm's law became the fundamental law in circuit analysis. In 1959, inventor Otis Boykin filed a patent for a resistor that allows manufacturers to designate a value of resistance for a piece of wire in equipment. In 1962, he patented an improved version, which could withstand more extreme conditions. This reduced the cost and increased the reliability of a variety of electronic products. <ref>{{cite web|work=The Philadelphia Tribune|title=Otis Boykin: Invented an Improved Electrical Resistor| publisher=The Philadelphia Tribune|url=http://www.phillytrib.com/otis-boykin-invented-an-improved-electrical-resistor/article_f73aeede-4d70-5ea2-90c6-4d8b7b93e3e1.html}}</ref>


What are the mathematical equations that allow us to model this topic.  For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.
==Mathematics==


===A Computational Model===
As discussed above, resistance of a material is dependent on two factors: the properties of the material, and the area of the resistor.


How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]
From the above factors, we get the following definition of resistance:
<math>R = \frac{L}{σ A}</math>


==Examples==
In this definition <math> L </math> is the length of the resistor, <math> A </math> is the cross-sectional area of the resistor, and <math> σ </math> is the conductivity of the material.
<math> σ </math> can be further broken down to show <math> σ = |q|nu </math>.


Be sure to show all steps in your solution and include diagrams whenever possible
==In A Circuit==


===Simple===
There is a change in potential energy across a resistor, which is useful when evaluating the loop rule in a circuit with resistors. The change in potential across a resistor is <math> I = \frac{ΔV}{R} </math>
===Middling===
Knowing this equation allows one to solve for <math> ΔV </math> if given <math>I</math> and either <math>R</math> or the components of <math>R</math> enumerated above.
===Difficult===


==Connectedness==
In the case of a circuit resistors, the loop rule might look something like:
#How is this topic connected to something that you are interested in?
<math> |emf| = I_{1}R_{1} + I_{2}R_{2}</math>
#How is it connected to your major?
#Is there an interesting industrial application?


==History==
==Equations Derived==
From the definition of resistance and the voltage potential formula discussed above, a number of useful equations can be derived and solved.
The first equation is <math> v = uE</math> where <math> E </math> is electron field , <math> u</math> as electron mobility, and <math> v</math> is drift speed.


Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.
This equation offers insight into the microscopic view of the resistor.  


== See also ==
The second equation that can be derived is <math> I = |q|nAv</math>.
This equation can be used, in addition to the above equation <math> I = \frac{ΔV}{R}</math> to solve for macroscopic properties of the resistor.


Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?
==Example Problems==
===Easy Example===


===Further reading===
'''Question:'''
Use the loop rule to calculate the voltage drop across each resistor. Then ensure that your answer is correct.
[[File:EasyExample.JPG]]


Books, Articles or other print media on this topic


===External links===


Internet resources on this topic
'''Answer:'''


==References==
[[File:EasyExampleAnswerResize.jpg]]


This section contains the the references you used while writing this page
===Difficult Example===
https://www.youtube.com/watch?v=BW7U_5BtH-8


[[Category:Which Category did you place this in?]]
==Applications==
'''1.How is this topic connected to something that you are interested in?''' I am very interested in computers and I know that circuitry is the foundation of computers and other electronic equipment.
 
'''2.How is it connected to your major?''' My major is Industrial Engineering, and although I won't study resistors directly in any of my classes, I understand that resistors are crucial in the creation of the tools all engineers and scientists use such as computers and calculators.
 
'''3.Is there an interesting industrial application?''' As stated above, resistors are widely used in electric circuits. They are used to reduce current flow, change signal levels, and terminate transmission.
 
==Bibliography==
<references> http://www.phillytrib.com/otis-boykin-invented-an-improved-electrical-resistor/article_f73aeede-4d70-5ea2-90c6-4d8b7b93e3e1.html <references/>

Latest revision as of 14:50, 27 November 2017

Claimed by Matthew Munns - Fall 2017

Resistors may exist in a circuit and resist electric charge. The resistance of a resistor depends on the properties of the material and the area of the resistor. These two attributes will be investigated later in the page.

Resistors may be ohmic or non-ohmic. An ohmic resistor has a conductivity that is nearly constant, while a non-ohmic resistor will vary depending on the conditions. This page will focus on ohmic resistors in a complex circuit.

The following is an image of an ohmic resistor like the resistor used in lab:

History

Georg Simon Ohm, born in 1789, discovered Ohm's law. This law relates the current, voltage, and resistance across a resistor. His law was widely accepted by 1850. Ohm's law became the fundamental law in circuit analysis. In 1959, inventor Otis Boykin filed a patent for a resistor that allows manufacturers to designate a value of resistance for a piece of wire in equipment. In 1962, he patented an improved version, which could withstand more extreme conditions. This reduced the cost and increased the reliability of a variety of electronic products. [1]

Mathematics

As discussed above, resistance of a material is dependent on two factors: the properties of the material, and the area of the resistor.

From the above factors, we get the following definition of resistance: [math]\displaystyle{ R = \frac{L}{σ A} }[/math]

In this definition [math]\displaystyle{ L }[/math] is the length of the resistor, [math]\displaystyle{ A }[/math] is the cross-sectional area of the resistor, and [math]\displaystyle{ σ }[/math] is the conductivity of the material. [math]\displaystyle{ σ }[/math] can be further broken down to show [math]\displaystyle{ σ = |q|nu }[/math].

In A Circuit

There is a change in potential energy across a resistor, which is useful when evaluating the loop rule in a circuit with resistors. The change in potential across a resistor is [math]\displaystyle{ I = \frac{ΔV}{R} }[/math] Knowing this equation allows one to solve for [math]\displaystyle{ ΔV }[/math] if given [math]\displaystyle{ I }[/math] and either [math]\displaystyle{ R }[/math] or the components of [math]\displaystyle{ R }[/math] enumerated above.

In the case of a circuit resistors, the loop rule might look something like: [math]\displaystyle{ |emf| = I_{1}R_{1} + I_{2}R_{2} }[/math]

Equations Derived

From the definition of resistance and the voltage potential formula discussed above, a number of useful equations can be derived and solved. The first equation is [math]\displaystyle{ v = uE }[/math] where [math]\displaystyle{ E }[/math] is electron field , [math]\displaystyle{ u }[/math] as electron mobility, and [math]\displaystyle{ v }[/math] is drift speed.

This equation offers insight into the microscopic view of the resistor.

The second equation that can be derived is [math]\displaystyle{ I = |q|nAv }[/math]. This equation can be used, in addition to the above equation [math]\displaystyle{ I = \frac{ΔV}{R} }[/math] to solve for macroscopic properties of the resistor.

Example Problems

Easy Example

Question: Use the loop rule to calculate the voltage drop across each resistor. Then ensure that your answer is correct.


Answer:

Difficult Example

https://www.youtube.com/watch?v=BW7U_5BtH-8

Applications

1.How is this topic connected to something that you are interested in? I am very interested in computers and I know that circuitry is the foundation of computers and other electronic equipment.

2.How is it connected to your major? My major is Industrial Engineering, and although I won't study resistors directly in any of my classes, I understand that resistors are crucial in the creation of the tools all engineers and scientists use such as computers and calculators.

3.Is there an interesting industrial application? As stated above, resistors are widely used in electric circuits. They are used to reduce current flow, change signal levels, and terminate transmission.

Bibliography

<references> http://www.phillytrib.com/otis-boykin-invented-an-improved-electrical-resistor/article_f73aeede-4d70-5ea2-90c6-4d8b7b93e3e1.html