Electric Force, Field, and Potential

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

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

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

$C=Q \times V$

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.

Diode

Resistor

Inductor

Capacitor

The brightness will decrease

The brightness will increase

The light bulb will change color

The brightness will remain unchanged

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.

It decreased the reliability of electronic circuits due to thermal instability.

It allowed for the miniaturization and increased precision of measurement tools.

It eliminated the need for analog technology in all scientific measurements and calculations.

It increased the overall power consumption of scientific instruments, reducing their efficiency.

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.

Thomson's cathode ray experiment

Rutherford's gold foil experiment

Davisson-Germer experiment

Millikan oil drop experiment

Ohm

Siemens

Farad

Tesla

Henry

Watt

Volt

Joule