Inside a conducting hemisphere shell, the electric field is zero because the charges redistribute themselves to cancel out any electric field. Outside the conducting hemisphere shell, the electric field behaves as if all the charge is concentrated at the center of the hemisphere.
The electric potential inside a conducting spherical shell is zero.
The electric potential inside an object made from a conducting material is zero.
The charge distribution on a conducting shell affects the electric field inside the shell. If the charge is distributed evenly, the electric field inside the shell is zero. If the charge is not evenly distributed, there will be an electric field inside the shell.
The electric field inside a charged insulator is zero, while the electric field outside a charged insulator is non-zero.
The electric potential inside a ring conductor on a conducting paper is zero because the electric field inside a conductor in electrostatic equilibrium is zero. This is due to the charges redistributing themselves in such a way that the electric field cancels out inside the conductor. Since the electric potential is directly related to the electric field, the potential inside the conductor is also zero.
The electric potential inside a conducting spherical shell is zero.
The electric potential inside an object made from a conducting material is zero.
The charge distribution on a conducting shell affects the electric field inside the shell. If the charge is distributed evenly, the electric field inside the shell is zero. If the charge is not evenly distributed, there will be an electric field inside the shell.
The electric field inside a charged insulator is zero, while the electric field outside a charged insulator is non-zero.
The electric potential inside a ring conductor on a conducting paper is zero because the electric field inside a conductor in electrostatic equilibrium is zero. This is due to the charges redistributing themselves in such a way that the electric field cancels out inside the conductor. Since the electric potential is directly related to the electric field, the potential inside the conductor is also zero.
In a conducting sheet, the electric field is zero inside the material but can exist on the surface due to excess charge redistribution. In a non-conducting sheet, the electric field can exist both inside the material and on the surface, depending on the charge distribution.
electric field inside the conducting sphere is ZER0..! because their are equivalent charges all around the sphere which makes the net force zero hence we can say that the electric field is also zero.!
well the answer is no but inside the body he forms electric. so i mean he doesn't have electric in the outside but he does in the inside
A spherical non-conducting shell has the following properties and characteristics: It has a spherical shape with a hollow interior. The material of the shell does not conduct electricity. The inner radius of the shell determines the size of the hollow space inside. The shell can have various thicknesses, but the inner radius is a key parameter in determining its properties. The electric field inside the shell is zero, regardless of the presence of any charges or electric fields outside the shell. The electric field outside the shell behaves as if all the charge is concentrated at the center of the shell.
The electric field is strongest close to the source charge and weakens with distance from the source. It is weaker in regions with insulating materials compared to regions with conducting materials. Additionally, the electric field is weaker inside a conductor compared to outside the conductor due to charge redistribution.
Inside a charged insulator, the electric field is 0, as charges cannot move freely in insulators. Outside the insulator, the electric field behaves as if all the charge is concentrated at the center of the insulator.
The distribution of the electric field within a non-conducting sphere is uniform, meaning it is the same at all points inside the sphere. This is because the electric field lines are evenly distributed in all directions from the center of the sphere.