Now consider four point charges, q1, q2, q3, and q4, that lie in the plane of the page as shown in the diagram above. Imagine a three-dimensional closed surface whose cross section in the plane of the page is indicated. i. Which of these charges contribute to the net electric flux through the surface? ii. Which of these charges contribute to the electric field at point P, ? iii. Are your answers to i and ii the same or are they different? Explain why this is so.

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Can you help me with part d of this homework its split into 3 parts but its technically one question

P1
•92
93
• 94
Now consider four point charges, q1, q2, q3, and q4, that lie in the plane of the page as shown in
the diagram above. Imagine a three-dimensional closed surface whose cross section in the plane
of the page is indicated.
i. Which of these charges contribute to the net electric flux through the surface?
ii. Which of these charges contribute to the electric field at point P ?
iii. Are your answers to i and ii the same or are they different? Explain why this is so.
Transcribed Image Text:P1 •92 93 • 94 Now consider four point charges, q1, q2, q3, and q4, that lie in the plane of the page as shown in the diagram above. Imagine a three-dimensional closed surface whose cross section in the plane of the page is indicated. i. Which of these charges contribute to the net electric flux through the surface? ii. Which of these charges contribute to the electric field at point P ? iii. Are your answers to i and ii the same or are they different? Explain why this is so.
Expert Solution
Step 1

i.  Gauss Law of electrostatics states that the electric flux through any hypothetical closed surface (irrespective of its shape and size) is equal to 1ε0times the net electric charge that the surface encloses

Going by Gauss Law , charges q2 and q3 will contribute to the net electric flux through the surface.

 

ii) All the the charges (q1, q2, q3 and q4) will contribute to the electric field.

Electric field due to more than one charge is vector sum total of the electric field due to individual charges. We apply the principle of superposition.

 

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