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An example of this (with sample values) is given in Figure 7.35. We could draw a similar set of equipotential isolines for gravity on the hill shown in Figure 7.2. If the hill has any extent at the same slope, the isolines along that extent would be parallel to each other. Furthermore, in regions of constant slope, the isolines would be evenly spaced. This equation tells us that the distance r from the point charge remains constant casino bigwins for all points on the equipotential surface. In other words, the equipotential surface for a point charge is a sphere centered at the charge, with a radius r given by the above equation.
An important application of electric fields and equipotential lines involves the heart. The movement of electrical signals causes the chambers of the heart to contract and relax. When a person has a heart attack, the movement of these electrical signals may be disturbed. An artificial pacemaker and a defibrillator can be used to initiate the rhythm of electrical signals.
The equation indicates that where the radius of curvature is large (points B and D in Figure 7.40), latex\sigma/latex and E are small. (c) Since the electric field is constant, find the ratio of 100 V to the total potential difference; then calculate this fraction of the distance. Expert educators at Vedantu always stress drawing correct diagrams, paying attention to perpendicularity between field lines and equipotentials, and being alert to traps—such as thinking two equipotential surfaces may cross (they never do). The surface, the locus of all points at the same potential, is known as the equipotential surface. No work is required to move a charge from one point to another on the equipotential surface. In other words, any surface with the same electric potential at every point is termed as an equipotential surface.
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For a point charge, equipotential surfaces are spheres centered on the charge. The equipotential surface concept builds clear links to other JEE topics like Gauss’s law, potential energy of electric dipole, and electrostatic potential and capacitance. Practice visualising and mapping surfaces for all typical configurations. Remember, electric field is always highest where equipotential surfaces are closest together. The surface charge density on a long straight metallic pipe is latex\sigma/latex. These have equipotential lines that are parallel to the plates in the space between and evenly spaced.
Therefore, the gradient always points normal to equipotential surfaces. A surface with an equipotential potential is one where all points on the surface have the same electric potential. This means that at every point on the equipotential surface, a charge will have the same potential energy. One of the most important cases is that of the familiar parallel conducting plates shown in Figure 7.35. Between the plates, the equipotentials are evenly spaced and parallel. The same field could be maintained by placing conducting plates at the equipotential lines at the potentials shown.
To improve your intuition, we show a three-dimensional variant of the potential in a system with two opposing charges. Figure 7.33 displays a three-dimensional map of electric potential, where lines on the map are for equipotential surfaces. The hill is at the positive charge, and the trough is at the negative charge. Note that the cut off at a particular potential implies that the charges are on conducting spheres with a finite radius. One of the rules for static electric fields and conductors is that the electric field must be perpendicular to the surface of any conductor.
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For example, grounding the metal case of an electrical appliance ensures that it is at zero volts relative to the earth. One of the uses of this fact is that a conductor can be fixed at what we consider zero volts by connecting it to the earth with a good conductor—a process called grounding. For example, grounding the metal case of an electrical appliance ensures that it is at zero volts relative to Earth.
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However, this contradicts the definition of an equipotential surface, which states that there is no potential difference between any two places on the surface and that no work is necessary to move a test charge over it. Therefore, at all points, the electric field must be normal to the equipotential surface. Equipotential surfaces allow an alternative visual image in addition to the image of electric field lines around a charge arrangement. As expected, in the region latexr\ge R,/latex the electric field due to a charge q placed on an isolated conducting sphere of radius R is identical to the electric field of a point charge q located at the center of the sphere. In Example 7.19 with a point charge, we found that the equipotential surfaces were in the form of spheres, with the point charge at the center. Given that a conducting sphere in electrostatic equilibrium is a spherical equipotential surface, we should expect that we could replace one of the surfaces in Example 7.19 with a conducting sphere and have an identical solution outside the sphere.
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