Question
Question: The voltage $V(t)$ across a capacitor of capacitance $C$ discharging through a resistance $R$ is giv...
The voltage V(t) across a capacitor of capacitance C discharging through a resistance R is given by V(t)=V0e−t/RC. The initial voltage V0 is 10.00 ± 0.02 V, R=100.0±0.1 MΩ and C=1.00 μF. The circuit is closed and subsequently disconnected after 100 ± 1 seconds. The final voltage is best represented as

2.71 ± 0.01 V
3.67 ± 0.003 V
3.67 ± 0.05 V
3.67 ± 0.37 V
3.67 ± 0.05 V
Solution
The voltage across a discharging capacitor is given by V(t)=V0e−t/RC.
Given values: Initial voltage V0=10.00±0.02 V Resistance R=100.0±0.1 MΩ=(100.0±0.1)×106 Ω Capacitance C=1.00 μF=1.00×10−6 F (Uncertainty in C is not given, so assume it's negligible) Time t=100±1 s
1. Calculate the nominal value of the final voltage V(t):
First, calculate the time constant τ=RC. τ=(100.0×106 Ω)×(1.00×10−6 F)=100.0 s
Now, substitute the values into the voltage equation: V(t)=V0e−t/RC=10.00×e−100/100.0=10.00×e−1 V(t)=10.00×0.36787944...≈3.67879 V Rounding to two decimal places, V(t)≈3.68 V. Looking at the options, 3.67 V is preferred.
2. Calculate the uncertainty in the final voltage ΔV:
The formula for error propagation for a function Y=f(X1,X2,…,Xn) is given by: (ΔY)2=(∂X1∂YΔX1)2+(∂X2∂YΔX2)2+⋯+(∂Xn∂YΔXn)2
In our case, V=V0e−t/RC. We need to find ΔV considering uncertainties in V0, t, and R. We assume ΔC=0.
The partial derivatives are: ∂V0∂V=e−t/RC ∂t∂V=V0e−t/RC(−RC1)=−RCV ∂R∂V=V0e−t/RC(−Ct)(−R−2)=VCR2t
Now, substitute these into the error propagation formula: (ΔV)2=(∂V0∂VΔV0)2+(∂t∂VΔt)2+(∂R∂VΔR)2 (ΔV)2=(e−t/RCΔV0)2+(−RCVΔt)2+(VCR2tΔR)2
Divide by V2 to get the relative uncertainty squared: (VΔV)2=(Ve−t/RCΔV0)2+(V−RCVΔt)2+(VVCR2tΔR)2 Since V=V0e−t/RC, the first term simplifies: Ve−t/RC=V0e−t/RCe−t/RC=V01. The last term simplifies: CR2tΔR=RCtRΔR.
So, (VΔV)2=(V0ΔV0)2+(RCΔt)2+(RCtRΔR)2
Now, calculate the relative uncertainties: V0ΔV0=10.000.02=0.002 tΔt=1001=0.01 RΔR=100.00.1=0.001
And the terms in the equation: t/RC=100/100=1 RCΔt=tΔt×RCt=0.01×1=0.01 RCtRΔR=1×0.001=0.001
Substitute these values into the equation for (VΔV)2: (VΔV)2=(0.002)2+(0.01)2+(0.001)2 (VΔV)2=0.000004+0.000100+0.000001 (VΔV)2=0.000105
Now, calculate VΔV: VΔV=0.000105≈0.01024695
Finally, calculate the absolute uncertainty ΔV: ΔV=V×(VΔV) Using V≈3.67879 V: ΔV=3.67879×0.01024695≈0.03769 V
Rounding ΔV to one or two significant figures, it is approximately 0.04 V or 0.038 V. The nominal voltage is 3.67879 V. If we round it to 3.67 V, then the uncertainty should be consistent. Comparing our result with the options: (A) 2.71 ± 0.01 V (B) 3.67 ± 0.003 V (C) 3.67 ± 0.05 V (D) 3.67 ± 0.37 V
Our calculated voltage is 3.67 V (or 3.68 V). Our calculated uncertainty is 0.03769 V. Option (C) has V=3.67 V and ΔV=0.05 V. This is the closest option to our calculated uncertainty. 0.03769 V rounded up to one significant figure for uncertainty would be 0.04 V. If we round to a multiple of 5 for simplicity, 0.05 V is a reasonable choice if the precision is lower.
Let's re-evaluate the rounding. Usually, the uncertainty is quoted to one or two significant figures. 0.03769≈0.038 or 0.04. The options are 0.003,0.05,0.37. 0.05 is the closest option to 0.038 or 0.04.
The final voltage is best represented as 3.67±0.05 V.