| Ampere’s Circular LawThe formula for Ampere’s circuital law  are as stated below | 
| Description | Formula | 
| Ampere’s circuital law | \int_{\ }^{\ }B.dl=μ°I
Here μ°= permeability of free space=4Π×10-15NA-2
B = Magnetic field
I = enclosed electric current by the path | 
| Ampere’s law (integral form) | \int_{\ }^{\ }B.ds=μ°Ienclosed
Ienclosed= enclosed current by the surface | 
| Field of a current-carrying wire: | B=μ°/I2πr | 
| Field of a solenoid | BL=°NI
Here N: number of turns in the solenoid | 
| Field inside a thick wire | \int B.ds=μ°I
And
B=μ°I.r2/πR2 | 
| Field of the toroid | B=μ°NI/2πr | 
| Force between two parallel current carrying wires | F_\frac{A}{B}=μ°IAIB2πr
IA,IB= Current carrying by wires A and B | 
| Capacitance formulaThe formula for capacitance are as stated below | 
| Description | Formula | 
| Capacitance of a parallel plate capacitor in terms of charge and potential difference | C=Q/V
Here, C is the capacitance of the capacitor, Q is the charge stored and V is the potential difference between the plates. | 
| Capacitance of a parallel plate capacitor in terms of surface area and distance between the plates | C=\frac{\varepsilon_0A}{d}
Here,  is the permittivity of free space and its value is 8.854×10-12m-3 Kg-1 s4 A2 is the surface area of the plates and d is the distance between the plates. | 
| Capacitance of a spherical capacitor derivation | To find the formula for capacitance of a spherical capacitor we will use the gauss’s law.
Let the charge on the spherical surface be , the radius of smaller sphere be  and radius of the bigger sphere be .
Using gauss’s law, we can write:
\oint_{\ }^{\ }\ \vec{E}\cdot d\vec{A}=\frac{Q}{\varepsilon_0}
E\left(4\pi r^2\right)=\frac{Q}{\varepsilon_0}
E=\frac{Q}{4\pi\varepsilon_0r^2}
V=\frac{Q}{4\pi\varepsilon_0r} | 
| The potential difference between the plates | V_{ab}=V_a-V_b=\frac{Q}{4\pi\varepsilon_0}\left(\frac{1}{r_a}-\frac{1}{r_b}\right)
=\frac{Q}{4\pi\varepsilon_0}\frac{r_b-r_a}{r_ar_b}
Therefore, the capacitance will be:
C=\frac{Q}{V_{ab}}=\ 4\pi\varepsilon_0\frac{r_ar_b}{r_b-r_a} | 
| Energy stored in capacitor | ● U=1/2 CV2
● U= Q2/2c
● U= QV/2
Here, U is the energy, C is the capacitance, V is the potential difference and Q is the charge stored. | 
| Energy density of capacitor | Energy density=\frac{1}{2}\varepsilon_0\varepsilon_rE^2
In vacuum:
Energy density= \frac{1}{2}\varepsilon_0E^2
Here, Eo is the permittivity of free space,  is the relative permittivity and E is the electric field. | 
| Capacitance per unit length of a cylindrical capacitor | Capacitance per unit length= 2ΠEo/In(b/a)
Here, Eo is the permittivity of free space, b is the radius of outer cylinder and a is the radius of inner cylinder. | 
| Electric field intensity | The formula for electric field intensity between the plates is given as:
E= σ/Eo=V/d
Here, σ is the surface charge density, V is the potential difference and d is the distance between plates. | 
| Redistribution of charge when two charged capacitors are connected in parallel | Let us assume a capacitor with capacitance  with initial charge  and capacitor with capacitance  with initial charge .
The final charge on capacitor with capacitance will be:
Q’1=C1/C1+c2(Q1+Q2)
final charge on capacitor with capacitance will be:
Q’2=C1/C1+c2(Q1+Q2) | 
| Equivalent capacitance when capacitors are connected in series | \frac{1}{C_{eq}}=\frac{1}{C_1}+\frac{1}{C_2}+\frac{1}{C_3}+\ldots+\frac{1}{C_n}
Here,  is the equivalent capacitance and  are the capacitance of the capacitors. | 
| Equivalent capacitance of the capacitors connected in parallel | C_{eq}=C_1+C_2+C_3+\ldots C_n | 
| Charging of capacitor | q=q_0\left(1-e^{-\frac{t}{\tau}}\right)
Here, q is the charge on the capacitor at time t,  is the time constant and  is the charge on the capacitor at steady state. | 
| Discharging of capacitor | q=q_0e^{-\frac{t}{\tau}}
Here, q is the charge on the capacitor at time t,  is the time constant and  is the charge on the capacitor at steady state. |