If unifrom electric filed `vecE = E_(0)hati + 2E_(0) hatj`, where `E_(0)` is a constant, exists in a region of space and at `(0, 0)` the electric potential `V` is zero, then the potential at `(x_(0),0)` will be.

If uniform electric field vec E = E_ 0 hati + 2 E _ 0 hatj , where E _ 0 is a constant exists in a region of space and at (0,0) the electric potential V is zero, then the potential at ( x _ 0 , 2x _ 0 ) will be -

If uniform electric field vec E = E_ 0 hati + 2 E _ 0 hatj , where E _ 0 is a constant exists in a region of space and at (0,0) the electric potential V is zero, then the potential at ( x _ 0 , 2x _ 0 ) will be -

If uniform electric field vec E = E_ 0 hati + 2 E _ 0 hatj , where E _ 0 is a constant exists in a region of space and at (0,0) the electric potential V is zero, then the potential at ( x _ 0 , _ 0 ) will be -

For a uniform electric field vecE = E_(0)(hati) , if the electric potential at x = 0 is zero, then the vaJut of electric potential at x = +x will be ..... .

Conisder an electric field vecE=E_0hatx where E_0 is a constant . The flux through the shaded area (as shown in the figure) due to this field is

Conisder an electric field vecE=E_0hatx where E_0 is a constant . The flux through the shaded area (as shown in the figure) due to this field is

Assum that an electric field vecE = 30 x^(2) hati exists in space. Then the potential difference V_(A) - V_(0) , where V_(0) the potential at the origin and V_(A) the potential at x = 2 m is :

An electric field vecE=10xhai i exists in a certain region of space. Then the potential difference V=V_(0)-V_(A) , where V_(0) is the potential at the origin and V_(A) is the potential at x =2 m is …….. .

Electric field strength vecE = E_0 hati and vecB = B_0 hati exists in a region. A charge is projected with a velocity vecv = v_0 hatj origin, then