Work each one out on paper first, then tap "show answer" to check. They get harder as you go, ending with the full combined circuit from the lab.
I = Q / t = 15 ÷ 5 = 3 A
Convert to seconds first: 3 minutes = 180 s.
Q = I × t = 2 × 180 = 360 C
V = W / Q = 45 ÷ 9 = 5 V
Rearrange V = W/Q to make W the subject: W = V × Q.
W = 9 × 8 = 72 J
V = I × R = 2.5 × 8 = 20 V
R = V / I = 15 ÷ 3 = 5 Ω
(a) Rtotal = 4 + 6 = 10 Ω
(b) I = V / R = 20 ÷ 10 = 2 A — this is the current everywhere in the loop
(c) V1 = I × 4 = 8 V · V2 = I × 6 = 12 V (check: 8 + 12 = 20 V ✓)
V1 = 8 V, V2 = 12 V
Both branches see the full 10 V.
(a) I1 = 10 ÷ 5 = 2 A · I2 = 10 ÷ 20 = 0.5 A
(b) Itotal = 2 + 0.5 = 2.5 A
(c) 1/Rp = 1/5 + 1/20 = 4/20 + 1/20 = 5/20, so Rp = 20/5 = 4 Ω (check: I = V/Rp = 10/4 = 2.5 A ✓)
I1 = 2 A, I2 = 0.5 A, Rp = 4 Ω
Rp = (2 × 2) / (2 + 2) = 4/4 = 1 Ω
Rtotal = 1 + 1 = 2 Ω
I = 9 ÷ 2 = 4.5 A
Vs = 4.5 × 1 = 4.5 V · Vp = 4.5 × 1 = 4.5 V (check: 4.5 + 4.5 = 9 V ✓)
Since both parallel resistors are equal, the current splits evenly: I1 = I2 = 4.5 ÷ 2 = 2.25 A
I = 4.5 A, I1 = I2 = 2.25 A
Predict: with the 1.0 Ω branch cut, all the current that used to split between two branches now has only one road left — the 2.5 Ω branch — so its current should increase. The voltmeter is wired straight across the battery terminals and draws no current, so it keeps reading the full EMF no matter what the branches are doing: it should stay at 12 V.
Check: with the 1.0 Ω branch open, current only flows through the 1.0 Ω series resistor and the 2.5 Ω branch: Rtotal = 1.0 + 2.5 = 3.5 Ω.
I = 12 ÷ 3.5 ≈ 3.4 A — up from 2.0 A before the fault, confirming the prediction.
2.5 Ω branch: 2.0 A → 3.4 A. Voltmeter: stays at 12 V.
Go to the lab and use the "Top branch" switch under Break the Circuit to see this exact scenario animate.