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Set 51 Problem number 6


Problem

A charge of 1 `microC is located at (-19.01 m,-15.01 m).  

Solution

The electric field at a point is the force per unit test charge, with the test charge located at the point.

We can assume a unit test charge--i.e., a charge of 1 C.

Generalized Solution

We imagine charges Q and q at respective positions (x1, y1) and (x2, y2) in the plane, with q the 'test charge'. We find the force per unit charge on q.

By the usual means,we find that the magnitude of the force on either charge is | F | = k |Q q | / r^2. The force F12 exerted on charge 1 by charge 2 is equal and opposite to the force F21 exerted on charge 2 by charge 1.  The x and y components of the force at (x2, y2) are therefore

F21y = `F21 (y2 - y1) / r, where r = `sqrt [ (x2 - x1)^2 + (y2 - y1)^2 ]. 

The electric field at (x2, y2) is the force per unit of test charge at that point: E = F21 / q. Putting all the above expressions together we obtain

= k Q q / ( (x2-x1)^2 + (y2 - y1)^2) * (x2 - x1) / `sqrt( (x2-x1)^2 + (y2 - y1)^2)

= k Q q * (x2 - x1) / ( (x2-x1)^2 + (y2 - y1)^2) ^ (3/2)

and

= k Q q / ( (x2-x1)^2 + (y2 - y1)^2) * (y2 - y1) / `sqrt( (x2-x1)^2 + (y2 - y1)^2)

=  k Q q * (y2 - y1) / ( (x2-x1)^2 + (y2 - y1)^2) ^ (3/2).

Explanation in terms of Figure(s), Extension

The figure below depicts the charges Q and q at points (x1,y1) and (x2,y2).

The second figure shows the force vector F12 broken into components.

Figure(s)

field_due_to_charge_at_point.gif (5003 bytes)

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