A semi-infinite wire of uniform linear charge density $\lambda$ is placed as shown in figure. The conical surface is of radius $R$ and height $h.$The electric flux through the curved surface of the cone is

Three point charges $+Q,-Q$ and $+2Q$ are placed at the vertices of an isosceles right angled triangle as shown in figure. The magnitude of electric field intensity produced by these charges at the middle point of hypotenuse is

On a non-conducting ring of radius $R,+q$ and $-q$ charges are uniformly distributed in two halves as shown in figure. The electric field intensity on its axis at a distance $d$ from its centre is given by $\overrightarrow{E}$, then

Two point charges $A$ and $B$ are placed on $X$-axis. Considering electric field $E$ is positive if directed in positive $X$-direction. Variation of electric field strength with distance $x$ is shown in figure for $x$ lying between the charges. Then the nature of charges $A$ and $B$ are respectively

A non-conducting square plate of side length $2a$ is uniformly charged with charge $Q$ and a point charge $q$ is placed at perpendicular distance $a$ as shown in figure. The electric force on the point charge due to plate is

An annular disc of inner radius $R$ and outer radius $2R$ has uniformly distributed charge $Q.$ Electric field strength at point $P$ is

A small electric dipole of dipole moment $p$ is placed perpendicular to an infinitely long wire of linear charge density $\lambda .$ The centre of dipole is at a distance $r$ from the wire as shown. The electric force on the dipole is

A dielectric slab is placed in uniform electric field $E$ as shown in figure. Then

A hemisphere of radius $R$ as shown in figure is uniformly charged with a surface charge density $\sigma .$ The electric field at the centre $C$ is