The electric potential VV is the electrostatic potential energy possessed by a test charge, divided by the value of the charge itself. It is thus a scalar quantity, measured in volts (1 V=1 J/C1\ \text{V} = 1\ \text{J/C}), which assigns to every point in space a number independent of the charge placed there. Its great advantage is precisely this: while the field E\vec{E} is a vector with three components, the potential condenses the same information into a single scalar. Knowing VV at every point is equivalent to knowing the field, because E\vec{E} can be obtained from the equipotential surfaces and vice versa.

Principle — Electric potential

The potential generated by a point charge QQ at distance rr is V=kQr\ev{V = k\,\frac{Q}{r}} The potential difference between two points AA and BB is the negative of the circulation of the field along a path joining them: VBVA=ABEdV_B - V_A = -\int_A^B \vec{E}\cdot \dd\vec{\ell}

The physical intuition is that of a landscape of heights: the potential plays the role of altitude and the charge that of the mass moving through it. A positive charge placed where VV is high possesses a great deal of potential energy, exactly like a stone at the top of a hill; left free, it tends to slide towards lower values of VV, converting potential energy into kinetic energy.

Key formula

V=kQrV = k\dfrac{Q}{r} Epot=qVE_\text{pot} = q\,V VBVA=kQ ⁣(1rB1rA)V_B - V_A = k\,Q\!\left(\dfrac{1}{r_B}-\dfrac{1}{r_A}\right)

The potential energy of a charge qq immersed in the potential VV is simply Epot=qVE_\text{pot} = qV: the potential is the energy per unit charge, and multiplying it by the actual charge gives the true energy. For the point charge, the potential difference between two distances rAr_A and rBr_B is written compactly as VBVA=kQ(1/rB1/rA)V_B - V_A = kQ\left(1/r_B - 1/r_A\right), which shows how VV decreases in magnitude with distance from the source and tends to zero at infinity.

Collegamenti

Argomenti: Campo elettrico e potenziale Concetti: Potenziale elettrico · Energia potenziale elettrostatica

Esercizi collegati: Potential difference and work · Drill: work in moving a charge · Two connected conducting spheres