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Question: Two point charges \( 4 \times {10^{ - 6}}C \) and \( 2 \times {10^{ - 6}}C \) are placed at the vert...

Two point charges 4×106C4 \times {10^{ - 6}}C and 2×106C2 \times {10^{ - 6}}C are placed at the vertices AA and BB of a right angled triangle ABCABC respectively. BB is the right angle, AC=2×102mAC = 2 \times {10^{ - 2}}m and BC=102mBC = {10^{ - 2}}m . Find the magnitude and direction of resultant electric intensity at CC ?

Explanation

Solution

To solve this question first we will draw the diagram and we will find the electric field at point AA by using the formula and similarly at point BB after that we will find the angle θ\theta because without θ\theta we will not be able to find the resultant magnitude and then we will use the vector sum to find the net resultant and after to find the direction means we have to find tanα\tan \alpha after finding we will get our required solution.
Magnitude of the electric field is given by:
E=kqr2E = \dfrac{{kq}}{{{r^2}}}
Where,
kk is electrostatic constant and its value is 9×1099 \times {10^9} ,
qq is the charge and
rr is the distance.

Complete answer:

According to the question,
Charge at point AA is 4×106C4 \times {10^{ - 6}}C and
Charge at point BB is 2×106C2 \times {10^{ - 6}}C .
Length, AC=2×102mAC = 2 \times {10^{ - 2}}m and
Length, BC=102mBC = {10^{ - 2}}m .
So, the electric field at point AA is given by,
E=kqr2E = \dfrac{{kq}}{{{r^2}}}
Now, substituting the above given values and solving,
EA=9×109×4×106(2×102m)2 EA=9×109×4×1064×104 EA=9×107N C1  {E_A} = \dfrac{{9 \times {{10}^9} \times 4 \times {{10}^{ - 6}}}}{{{{\left( {2 \times {{10}^{ - 2}}m} \right)}^2}}} \\\ \Rightarrow {E_A} = \dfrac{{9 \times {{10}^9} \times 4 \times {{10}^{ - 6}}}}{{4 \times {{10}^{ - 4}}}} \\\ \Rightarrow {E_A} = 9 \times {10^7}N{\text{ }}{C^{ - 1}} \\\
Similarly, the electric field at point BB is given by,
E=kqr2E = \dfrac{{kq}}{{{r^2}}}
Now, substituting the above given values and solving,
EB=9×109×2×106(102m)2 EB=9×109×2×106104 EB=18×107N C1  {E_B} = \dfrac{{9 \times {{10}^9} \times 2 \times {{10}^{ - 6}}}}{{{{\left( {{{10}^{ - 2}}m} \right)}^2}}} \\\ \Rightarrow {E_B} = \dfrac{{9 \times {{10}^9} \times 2 \times {{10}^{ - 6}}}}{{{{10}^{ - 4}}}} \\\ \Rightarrow {E_B} = 18 \times {10^7}N{\text{ }}{C^{ - 1}} \\\
Now, we have to calculate the magnitude of resultant electric intensity at CC
To find this first we have to find the angle θ\theta .
In ABC\vartriangle ABC
cosθ=1022×102=12\cos \theta = \dfrac{{{{10}^{ - 2}}}}{{2 \times {{10}^{ - 2}}}} = \dfrac{1}{2}
And we know that, cos60=12\cos {60^ \circ } = \dfrac{1}{2}
Therefore, θ=60\theta = {60^ \circ }
Now, applying vector law of addition to find the magnitude,
E=EA+EB+2EAEBcosθE = \sqrt {{E_A} + {E_B} + 2{E_A}{E_B}\cos \theta }
Now, substituting all the values in above formula,
E = \sqrt {{E_A} + {E_B} + 2{E_A}{E_B}\cos \theta } \\\ \Rightarrow E = \sqrt {{{\left( {9 \times {{10}^7}} \right)}^2} + {{\left( {18 \times {{10}^7}} \right)}^2} + \left\\{ {2 \times 9 \times {{10}^7} \times 18 \times {{10}^7}\left( {\dfrac{1}{2}} \right)} \right\\}} \\\ \Rightarrow E = \sqrt {81 \times {{10}^{14}} + 324 \times {{10}^{14}} + 162 \times {{10}^{14}}} \\\
On further solving,
E=81×1014+324×1014+162×1014 E=547×1014 E=2.38×108N C1  E = \sqrt {81 \times {{10}^{14}} + 324 \times {{10}^{14}} + 162 \times {{10}^{14}}} \\\ \Rightarrow E = \sqrt {547 \times {{10}^{14}}} \\\ \Rightarrow E = 2.38 \times {10^8}N{\text{ }}{C^{ - 1}} \\\
So, the magnitude of resultant electric intensity at CC is 2.38×108N C12.38 \times {10^8}N{\text{ }}{C^{ - 1}} .
Now, we have to find the direction of the electric field at point CC .
Which, is nothing but tanα\tan \alpha
And is given by,
tanα=EBsinθEA+EBcosθ\tan \alpha = \dfrac{{{E_B}\sin \theta }}{{{E_A} + {E_B}\cos \theta }}
Now, substituting the values and solving we get,
tanα=18×107sin609×107+18×107cos60 tanα=18×107×329×107+9×107 tanα=32 α=40.9  \tan \alpha = \dfrac{{18 \times {{10}^7}\sin {{60}^ \circ }}}{{9 \times {{10}^7} + 18 \times {{10}^7}\cos {{60}^ \circ }}} \\\ \Rightarrow \tan \alpha = \dfrac{{18 \times {{10}^7} \times \dfrac{{\sqrt 3 }}{2}}}{{9 \times {{10}^7} + 9 \times {{10}^7}}} \\\ \Rightarrow \tan \alpha = \dfrac{{\sqrt 3 }}{2} \\\ \Rightarrow \alpha = {40.9^ \circ } \\\
Hence, the magnitude and direction of resultant electric intensity at CC is 2.38×108N C12.38 \times {10^8}N{\text{ }}{C^{ - 1}} and 40.9{40.9^ \circ } respectively.

Note:
It's important to remember that the electric field is defined as the force per unit of charge. Coulomb's Law states that the force between two charged particles is directly proportional to the charges and inversely proportional to the square of the distance between the charged particles, hence this value of electric field can be calculated. Keep in mind that in the case of positive charge, the electric field is radially outward, whereas in the case of negative charge, it is radially inward.