Electric Force, Field, and Potential

$C=\frac{V}{Q}$

$C=\frac{Q}{V}$

$C=k\frac{Q}{V}$

$C=Q \times V$

Diode

Resistor

Inductor

Capacitor

The brightness will decrease

The brightness will increase

The light bulb will change color

The brightness will remain unchanged

Change the plate area while keeping separation constant, using a single dielectric material and measuring energy stored.

Measure capacitance with varying dielectric constants, ensuring plates are significantly larger than separation distance to minimize fringe effects.

Use different battery voltages to charge capacitors with identical dielectrics, measuring the time constant for each.

Vary plate separation with a fixed voltage across capacitors without any dielectric to observe changes in capacitance.

Simulate idealized sphere charge distribution models excluding real-world physical boundary conditions.

Directly apply Potential difference between center sphere surface points neglecting any possible end effects.

Compare calculated values from Poisson's equation solutions using average surface charge densities instead of exact distributions.

Offset measurements away from surface extremities by using finely tuned sensors capable of high precision local electric field detection.

Charges move continuously within the conductor.

No charges are present on a conductor at equilibrium.

Charges are uniformly distributed throughout the volume.

Charges reside on the surface.

It leaves total resistance unchanged if resistors are identical.

It increases the total resistance.

It decreases the total resistance.

There's no general rule; it depends on other components' values too.

Ohm

Siemens

Farad

Tesla

Reduction in the quantity of electrons emitted with decreasing wavelength.

Ejection of electrons at specific threshold frequency regardless intensity.

Cumulative heating effect on metal surface with prolonged exposure to light.

Increase in kinetic energy of photoelectrons with light intensity.

Ampere

Volt

Coulomb

Ohm