what is the geometrical shape of equipotential surface due to single isolated charge
Equipotentials cannot cross because they relate to places with a given value for potential. Lines of force meet at the charge or point of mass. They can cross if they relate to the same potential. Think of two mountain chains of unvarying height crossing each-other.
Some practical real world examples why surface area is important:If you want to paint a house, you need to know the surface area to determine how much paint to buy.If you want to plant grass on a dirt lot, you need to know the surface area to determine how much grass seat to use.If you want to sew a dress, you need to know the surface area of the dress (dress size) to know how much material you need.If you want to make money mowing lawns, you need to know the surface area of the lawn to know how much to charge for the work.If you want to put carpet in a living room, you need to know the surface area of the room to know how much carpet you will need.If you are making a label for a soup can company, you will need to know the surface area of the can.
I charge $5 per foot with a 100 ft min.
The electron domain charge cloud geometry of ICI5 s usually positively charged. This is because the process involves the loss of electrons. The electron-domain charge-cloud geometry of ICl5 is octahedral.
Octahedral
concentric spherical surfaces
yes
No work is done when moving a charge on an equipotential surface because the potential remains constant. The work done is zero.
No work is done in moving a unit positive charge through a distance x on an equipotential surface. This is because an equipotential surface has a constant electric potential, and work done is equal to the charge multiplied by the change in potential. Since the potential is constant, there is no change in potential and thus no work done.
Equipotential refers to a surface where all points have the same electrical potential. In physics, this means that the work done in moving a charge from one point to another along that surface is zero. Equipotential surfaces are used to visualize and analyze electric fields.
A conductor is an equipotential surface because the electric field inside a conductor is zero in electrostatic equilibrium. This means that all points on the conductor have the same electric potential, making it an equipotential surface. Any excess charge on the conductor redistributes itself to ensure this equal potential.
The work done in moving a charge on an equipotent surface is zero. This is because the potential is constant along equipotential surfaces, so there is no change in potential energy as the charge moves between points on the surface. Therefore, the work done is zero.
An equipotential surface in the context of electric fields is significant because it represents points that have the same electric potential. This means that no work is required to move a charge along an equipotential surface, making it a useful tool for understanding the behavior of electric fields and the distribution of charges in a given space.
An equipotential surface is a surface where all points have the same electric potential. In the context of electric fields, it signifies that no work is required to move a charge along that surface, as the electric field is perpendicular to the surface. This helps in visualizing the electric field lines and understanding the distribution of electric potential in a given region.
Moving a charge along an equipotential line does not affect its potential energy. This is because equipotential lines represent points of equal potential, so the potential energy of the charge remains constant along these lines.
In electrostatic equilibrium, the inside of a conductor is equipotential. This means that the electric potential is constant at all points within the material of the conductor. Any excess charge on the surface of the conductor would redistribute itself to ensure that the entire interior remains at the same potential.
The locus of points where the potential due to an isolated point charge is constant is a spherical surface centered on the point charge. This is because the potential decreases with distance from the point charge, so points at the same distance will have the same potential.