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<h2 class="hd hd-2 unit-title">Textbook Links</h2>
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<p> This first lesson introduces electric charge and the forces between electric charges.</p><p> Textbook Links </p><ul><li> Chapter 2: Coulomb's Law <a href="/courses/course-v1:MITx+8.02.1x+1T2019/pdfbook/0/chapter/2/3"><i class="it">chapter 2, sections 1-3</i></a></li></ul>
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<h2 class="hd hd-2 unit-title">L1v1: What is Charge</h2>
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<h3 class="hd hd-2">L01v01: What is Charge</h3>
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<h2 class="hd hd-2 unit-title">L1Q1: Electric Charge Properties. </h2>
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Electric Charge
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<p>Which of the following statements about electric charge is (are) true?</p>
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<text>a) It is conserved</text>
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<text>b) Like kinds of electric charge attract; unlike repel each other</text>
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<text>c) Electric charge can be of arbitrarily small amounts</text>
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<text>d) There are two kinds, negative and positive</text>
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<text>e) Electric charge can be quantified</text>
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Charge is Conserved
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<p>In the statement "Electric charge is conserved" what does "conserved" mean?</p>
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<text>a) A charged object will always remain charged.</text>
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<text>b) The sum of negative charges in the Universe does not change.</text>
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<text>c) The number of negative and positive charges in the Universe does not change.</text>
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<text>d) The total sum of the positive charges in the Universe does not change.</text>
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<text>e) The total sum of the negative and positive charge in the Universe does not change.</text>
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Charge is Quantized
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<p>In the statement "Electric charge is quantized" what does "quantized" mean?</p>
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<text>a) A charged object has a definite quantity of charge.</text>
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<text>b) The charge on an object can be measured in quants.</text>
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<text>c) Charge can be measured and described quantitatively in SI units.</text>
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<text>d) All charges that we can observe directly are integer multiples of some smallest possible amount of charge.</text>
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<text>e) The coulomb is the basic unit of electricity.</text>
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<h2 class="hd hd-2 unit-title">L1v2: Electric Force</h2>
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<h2 class="hd hd-2 unit-title">L1Q2: Units of the Coulomb Constant.</h2>
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Units of the Coulomb Constant
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Consider two point objects of charges [mathjaxinline]q_1&lt;0[/mathjaxinline] and [mathjaxinline]q_2&gt;0[/mathjaxinline] separated a distance [mathjaxinline]r[/mathjaxinline]. The electrostatic force exerted by object 2 on object 1 is given by Coulomb's law: </p>
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[mathjaxinline]\displaystyle \displaystyle \vec{F}_{2,1} = k\frac{q_1q_2}{r^2}\hat{r}_{2,1}[/mathjaxinline]
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where [mathjaxinline]\hat{r}_{2,1}[/mathjaxinline] is the unit vector directed along the line joining the two objects pointing from charge 2 to charge 1, and [mathjaxinline]k[/mathjaxinline] is the Coulomb constant. The value of the Coulomb constant in SI units is approximately [mathjaxinline]9\times 10^9[/mathjaxinline] and the units are: </p>
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<text> [mathjaxinline]k \approx 9\times 10^9 \frac{\mbox{N}\cdot \mbox{C}^2}{\mbox{m}^2}[/mathjaxinline]</text>
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<text> [mathjaxinline]k \approx 9\times 10^9 \frac{\mbox{N}\cdot \mbox{m}^2}{\mbox{C}^2}[/mathjaxinline]</text>
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<text> [mathjaxinline]k \approx 9\times 10^9 \frac{\mbox{C}^2\cdot \mbox{m}^2}{\mbox{N}}[/mathjaxinline]</text>
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<text> [mathjaxinline]k \approx 9\times 10^9 \frac{\mbox{N}\cdot \mbox{m}}{\mbox{C}^2}[/mathjaxinline]</text>
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<h2 class="hd hd-2 unit-title">L1v3: Rewrite the Unit Vector in Coulomb's Law</h2>
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<p><b>Unit vectors and Coulomb's law. </b></p><p><center><img src="/assets/courseware/v1/907131dd83f657d4bef68fb58a4cb129/asset-v1:MITx+8.02.1x+1T2019+type@asset+block/images_html_lesson1_unit_vectors_a.svg" width="300"/></center></p><p>Consider two objects of charges \(q_1\) and \(q_2\) shown in the figure above, \(\hat{r}_{1,2}\) is the unit vector directed along the line joining the two object that points from object 1 to object 2.</p><p><center><img src="/assets/courseware/v1/65f61430e8359160e1762742c2d9bbce/asset-v1:MITx+8.02.1x+1T2019+type@asset+block/images_html_lesson1_unit_vectors_b.svg" width="300"/></center></p><p> If \(\vec{r}_{1,2}\) is the position of object 2 measured from 1, shown above, the unit vector, \(\hat{r}_{1,2}\) can be expressed as:</p><p> \[\displaystyle \hat{r}_{1,2} = \frac{\vec{r}_{1,2}}{|\vec{r}_{1,2}|}\]</p><p>The electrostatic force exerted by object 1 on 2 is expressed in terms of the unit vector \(\hat{r}_{1,2}\) as:</p><p>
\[\displaystyle \vec{F}_{1,2} = kq_1q_2\frac{\hat{r}_{1,2}}{|\vec{r}_{1,2}|^2}\]
</p><p>and in terms of the vector \(\vec{r}_{1,2}\) the Coulomb force is given by:</p><p>
\[\displaystyle \vec{F}_{1,2} = kq_1q_2\frac{\vec{r}_{1,2}}{|\vec{r}_{1,2}|^3}\]
</p><p><b>Note:</b> In the second expression, the force is divided by the distance cubed but the magnitude of the force still follows an inverse square distance law.</p>
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<h3 class="hd hd-2">L01v03: Rewrite the Unit Vector in Coulomb's Law</h3>
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<h2 class="hd hd-2 unit-title">L1Q3: Unit Vector Calculation and Force Between two Charges.</h2>
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Unit vector calculation.
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Two charged objects are separated a distance [mathjaxinline]d[/mathjaxinline] as shown. The angle between the line joining the objects and the horizontal is [mathjaxinline]30^\circ[/mathjaxinline]. Consider the (x,y) coordinate system with origin at the location of object 2. </p>
<p><b class="bfseries">(Part a)</b> Calculate [mathjaxinline]\vec{r}_{2,1}[/mathjaxinline], the position vector of object 1 measured from object 2. Express your answer in terms of hati for [mathjaxinline]\hat{i}[/mathjaxinline], hatj for [mathjaxinline]\hat{j}[/mathjaxinline], and [mathjaxinline]d[/mathjaxinline] as needed. Remember that the argument of [mathjaxinline]\sin[/mathjaxinline] and [mathjaxinline]\cos[/mathjaxinline] in answer boxes needs to be entered in radians. <p style="display:inline">[mathjaxinline]\vec{r}_{2,1}=[/mathjaxinline]</p> <div class="inline" tabindex="-1" aria-label="Question 1" role="group"><div id="inputtype_checkpoint_w1_13_2_1" class="text-input-dynamath capa_inputtype inline textline">
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<p><b class="bfseries">(Part b)</b> Calculate [mathjaxinline]\hat{r}_{2,1}[/mathjaxinline], the unit vector pointing in the direction from object 2 to object 1. Express your answer in terms of hati for [mathjaxinline]\hat{i}[/mathjaxinline], hatj for [mathjaxinline]\hat{j}[/mathjaxinline], and [mathjaxinline]d[/mathjaxinline] as needed. <p style="display:inline">[mathjaxinline]\hat{r}_{2,1}=[/mathjaxinline]</p> <div class="inline" tabindex="-1" aria-label="Question 2" role="group"><div id="inputtype_checkpoint_w1_13_3_1" class="text-input-dynamath capa_inputtype inline textline">
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<p><b class="bfseries">(Part c)</b> Calculate the force on object 1 due to the interaction with object 2. Express your answer in terms of hati for [mathjaxinline]\hat{i}[/mathjaxinline], hatj for [mathjaxinline]\hat{j}[/mathjaxinline], [mathjaxinline]d[/mathjaxinline], [mathjaxinline]k[/mathjaxinline], q_1 for [mathjaxinline]q_1[/mathjaxinline] and q_2 for [mathjaxinline]q_2[/mathjaxinline] as needed. <p style="display:inline">[mathjaxinline]\vec{F}_{2,1}=[/mathjaxinline]</p> <div class="inline" tabindex="-1" aria-label="Question 3" role="group"><div id="inputtype_checkpoint_w1_13_4_1" class="text-input-dynamath capa_inputtype inline textline">
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<h2 class="hd hd-2 unit-title">Superposition of Coulomb's Law.</h2>
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<p><b>Superposition Principle. </b></p><p>Coulomb's law applies to any pair of point charges. When more than two charges are
present, the total force on any one charge is the vector sum of the forces exerted on
it by the other charges. For example, if three charges \(q_1\), \(q_2\) and \(q_3\) are present, the resultant force experienced by charge charge 3 is: .</p><p>
\[ \vec{F}_{3} = \vec{F}_{1,3} + \vec{F}_{2,3} \]
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<h2 class="hd hd-2 unit-title">L1v4: Worked Example - Total Force on a Charged Object</h2>
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Worked Example: Total force on a charged object.
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Three charged objects of charges [mathjaxinline]q_1[/mathjaxinline], [mathjaxinline]q_2[/mathjaxinline] and [mathjaxinline]q_3[/mathjaxinline] are located at the vertices of an isosceles triangles of base [mathjaxinline]2s[/mathjaxinline] and height [mathjaxinline]d[/mathjaxinline]. Assume [mathjaxinline]q_1=q_3=+Q[/mathjaxinline] and [mathjaxinline]q_2=-Q[/mathjaxinline], where [mathjaxinline]Q &gt;0[/mathjaxinline]. </p>
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Calculate, [mathjaxinline]\vec{F}_{2}[/mathjaxinline], the force exerted by objects 1 and 3 on object 2. Express your answer in terms of [mathjaxinline]k[/mathjaxinline], [mathjaxinline]Q[/mathjaxinline], [mathjaxinline]s[/mathjaxinline], [mathjaxinline]d[/mathjaxinline], hati for [mathjaxinline]\hat{i}[/mathjaxinline] and hatj for [mathjaxinline]\hat{j}[/mathjaxinline] as needed. </p>
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<p style="display:inline">[mathjaxinline]\vec{F}_{2}=[/mathjaxinline]</p>
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<h3 class="hd hd-2">L01v04: Worked Example - Total Force on a Charged Object</h3>
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<h2 class="hd hd-2 unit-title">L1Q4: Direction of the Total Force.</h2>
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Direction of the Total Force
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Three point-like charged objects are fixed on three corners of a square of side [mathjaxinline]a[/mathjaxinline]. The object at point [mathjaxinline]A[/mathjaxinline] has charge [mathjaxinline]-Q[/mathjaxinline], the object at point [mathjaxinline]B[/mathjaxinline] has charge [mathjaxinline]+Q[/mathjaxinline], and the object at point [mathjaxinline]C[/mathjaxinline] has charge [mathjaxinline]+Q[/mathjaxinline]. </p>
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Which of the arrows below best represents the approximate direction of the total force on the charge at point [mathjaxinline]C[/mathjaxinline]? </p>
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<h2 class="hd hd-2 unit-title">L1Q5: Charges on a Triangle.</h2>
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Charges on a triangle.
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Three point like objects of charges [mathjaxinline]q_1=-2q[/mathjaxinline], [mathjaxinline]q_2=+q[/mathjaxinline], and [mathjaxinline]q_3=-q[/mathjaxinline] (where [mathjaxinline]q[/mathjaxinline] is positive) are glued to the vertices of an equilateral triangle of side [mathjaxinline]a[/mathjaxinline] as shown. Consider the coordinate system indicated in the figure. </p>
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Calculate, [mathjaxinline]\vec{F}_{3}[/mathjaxinline], the force exerted by objects 1 and 2 on object 3. Express your answer in terms of [mathjaxinline]k[/mathjaxinline], [mathjaxinline]q[/mathjaxinline], [mathjaxinline]a[/mathjaxinline], hati for [mathjaxinline]\hat{i}[/mathjaxinline] and hatj for [mathjaxinline]\hat{j}[/mathjaxinline] as needed. </p>
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<p style="display:inline">[mathjaxinline]\vec{F}_{3}=[/mathjaxinline]</p>
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<h2 class="hd hd-2 unit-title">L1Q6: Gravitational Force vs. Electric Force. </h2>
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Gravitational force vs. electric force.
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The goal of this question is to compare [mathjaxinline]|\vec{F}_ G|[/mathjaxinline], the magnitude of the gravitational attraction between two protons with [mathjaxinline]|\vec{F}_ E|[/mathjaxinline], the magnitude of the electrostatic repulsion between them. </p>
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You might find the following constants useful: the mass of a proton [mathjaxinline]m_ p= 1.67\times 10^{-27}\; \mbox{kg}[/mathjaxinline], the gravitational constant [mathjaxinline]G= 6.67\times 10^{-11\, } \mbox{N}\; \mbox{m}^2\; \mbox{kg}^{-2}[/mathjaxinline], the charge of the proton [mathjaxinline]e= 1.6 \times 10^{-19} \mbox{C}[/mathjaxinline], and the Coulomb constant [mathjaxinline]k=9\times 10^9 \; \mbox{N}\; \mbox{m}^2\; \mbox{C}^{-2}[/mathjaxinline]. </p>
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Consider two protons a distance [mathjaxinline]d=10^{-15} \mbox{m}[/mathjaxinline] apart, the order of magnitude of the ratio [mathjaxinline]|\vec{F}_ G|/|\vec{F}_ E|[/mathjaxinline] is: </p>
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<text> [mathjaxinline]|\vec{F}_ G|/|\vec{F}_ E|\approx 10^{6}[/mathjaxinline]</text>
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