Uploaded by Michael Lee

Equations sheet

advertisement
πœ‡
𝑛
𝑝
10−6
10−9
10−12
Name
Current
Total charge
Negative terminal
𝐼
Δπ‘ž
Positive terminal
Resistance
Ohm's Law
𝐼=
Δπ‘ž
Δ𝑑
𝐴=
Δπ‘ž = 𝐼Δ𝑑
π›₯π‘‰π‘π‘Žπ‘‘
πœ€
𝑅
Rate at which energy is transferred from
the battery to the moving charges
Power delivered by a source of emf
Rate at which energy is transferred from
the current to the resistor
Kirchhoffs loop
law
Series Resistors
Parallel Resistors
Series Capacitors
πΆπ‘œπ‘’π‘™
𝑉 =0; π‘ˆ =0
π›₯π‘ˆ = π‘žπ›₯π‘‰π‘π‘Žπ‘‘
The potential difference of (over) a battery
= the potential difference of (over) a battery with
no current
π›₯π‘‰π‘π‘Žπ‘‘ slightly < πœ€ when with a current
𝑅=𝜌
𝐿
𝐴
𝐼 = Δ𝑉 𝑅
π‘ƒπ‘π‘Žπ‘‘ = Δπ‘ˆΔ𝑑 = Δπ‘žΔ𝑑 πœ€
π‘ƒπ‘’π‘šπ‘“ = 𝐼 πœ€
𝑃𝑅 = Δπ‘ˆΔ𝑑 = Δπ‘žΔ𝑑 Δ𝑉𝑅 = 𝐼 Δ𝑉𝑅
𝑃𝑅 = π‘ƒπ‘π‘Žπ‘‘
Kirchhoff's junction law
πΆπ‘œπ‘’π‘™
𝑠𝑒𝑐
𝑉 = π›₯π‘‰π‘π‘Žπ‘‘ ; π‘ˆ = π‘žπ›₯π‘‰π‘π‘Žπ‘‘
Energy gained
Electromotive force
SI Unit
Symbol
𝑃𝑅 = 𝐼 Δ𝑉𝑅 = 𝐼 2 𝑅 =
οΏ½ 𝐼𝑖𝑛 = οΏ½ πΌπ‘œπ‘’π‘‘
π‘‚β„Žπ‘š
π‘Š=
(Δ𝑉𝑅 )2
𝑅
Δπ‘‰π‘™π‘œπ‘œπ‘ = οΏ½ Δ𝑉𝑖 = 0
𝑖
Δπ‘‰π‘π‘Žπ‘‘ = πœ€ > 0 ; Δ𝑉𝑅 = −𝐼𝑅 < 0
π‘…π‘’π‘ž = 𝑅1 + 𝑅2 + β‹―
−1
1
1
π‘…π‘’π‘ž = οΏ½ +
+ β‹―οΏ½
𝑅1 𝑅2
πΆπ‘’π‘ž
−1
1
1
= οΏ½ + + β‹―οΏ½
𝐢1 𝐢2
1
𝐽
𝑠
Download