The electric field inside an infinitely long cylindrical conductor with radius r and uniform surface charge density is zero.
The electric field inside a conductor is zero, and the surface charge resides on the outer surface of the conductor. This means that the electric field at the surface of a conductor is perpendicular to the surface and proportional to the surface charge density.
The charge density for a conductor is zero in the bulk of the material when it is in electrostatic equilibrium. Any excess charge resides on the surface of the conductor. This is due to the principle that charges in a conductor distribute themselves in such a way that the electric field inside is zero.
Current density is the amount of electric current flowing through a given area. It is calculated by dividing the current passing through a conductor by the cross-sectional area of the conductor. The formula for current density is J I/A, where J is the current density, I is the current, and A is the cross-sectional area.
Concrete is a poor conductor of electricity, as it is not a metal and does not contain free-moving electrons that can carry electric charge effectively. However, it can conduct heat due to its density and composition.
The resistivity of a conductor is inversely proportional to the number density (n) of free electrons. This means that as the number density of free electrons increases, the resistivity of the conductor decreases, and vice versa. This relationship is due to the fact that more free electrons provide more paths for the flow of electric current, resulting in lower resistance.
The electric field inside a conductor is zero, and the surface charge resides on the outer surface of the conductor. This means that the electric field at the surface of a conductor is perpendicular to the surface and proportional to the surface charge density.
The charge density for a conductor is zero in the bulk of the material when it is in electrostatic equilibrium. Any excess charge resides on the surface of the conductor. This is due to the principle that charges in a conductor distribute themselves in such a way that the electric field inside is zero.
Density = Mass/Volume.
Current density is the amount of electric current flowing through a given area. It is calculated by dividing the current passing through a conductor by the cross-sectional area of the conductor. The formula for current density is J I/A, where J is the current density, I is the current, and A is the cross-sectional area.
Concrete is a poor conductor of electricity, as it is not a metal and does not contain free-moving electrons that can carry electric charge effectively. However, it can conduct heat due to its density and composition.
The conductor will not gain any charge that is not placed on it by you. However, the electric field will displace the free charges already within the conductor (by its nature) such that there will be a non-uniform surface charge density. Remember: a conductor must have zero electric field inside it, so the charges rearrange to cancel the external E-field. Again, this only repositions the existing charge, but it does not add or remove any charge.
The resistivity of a conductor is inversely proportional to the number density (n) of free electrons. This means that as the number density of free electrons increases, the resistivity of the conductor decreases, and vice versa. This relationship is due to the fact that more free electrons provide more paths for the flow of electric current, resulting in lower resistance.
On an irregularly shaped conductor, the surface charge density is greater at locations where the radius of curvature is smallest due to the electric field created by the surface charges. According to Gauss's law, the electric field strength is inversely proportional to the radius of curvature; sharper points or edges (smaller radius) produce a stronger electric field. To maintain electrostatic equilibrium, this results in a higher concentration of charge at these points, leading to greater surface charge density where the curvature is smallest. Thus, the distribution of charge is not uniform, reflecting the geometry of the conductor.
The drift velocity of free electrons in a conductor is directly proportional to the magnitude of the electric current flowing through the conductor. This means that as the current increases, the drift velocity of the electrons also increases. The relationship is described by the equation I = nAvq, where I is the current, n is the number density of charge carriers, A is the cross-sectional area of the conductor, v is the drift velocity, and q is the charge of the charge carrier.
The symbol for current density is typically denoted as J. It represents the amount of electric current flowing per unit area of a conductor and is measured in amperes per square meter (A/m²). Current density provides insight into how densely packed the electric current is in a given area, which is crucial for understanding electrical conductivity and circuit behavior.
Yes. They are infinitely dense. That is, there are infinitely many rational number between any two numbers.
*Electrical conductivity or specific conductivity [sigma] is a measure of a material's ability to conduct an electric current. When an electrical potential difference is placed across a conductor, its movable charges flow, giving rise to an electric current. The conductivity σ is defined as the ratio of the current density J to the electric field strength E : J=Sigma.E