CAIE A-Level Physics A2 19 Capacitance Questions
Practise analysing capacitance, series or parallel combinations, stored energy, discharge curves, time constants and exponential decay.
- Syllabus
- 2028–2030
- Course
- Physics 9702
- Level
- A2
Practise analysing capacitance, series or parallel combinations, stored energy, discharge curves, time constants and exponential decay.
An isolated conducting sphere in a vacuum has radius r and is initially uncharged. It is then charged by friction so that it carries a final charge Q. This charge can be considered to be acting at the centre of the sphere.
By considering the electric potential at its surface, show that the capacitance C of the sphere is given by
where ε0 is the permittivity of free space.
C=Q / V
V=Q/(4πε0r) and so C=Q/[Q/(4πε0r)]=4πε0r
The variation with potential difference V of the charge Q on one of the plates of a capacitor is shown in Fig. 5.1.
Fig. 5.1
The capacitor is connected to an 8.0 V power supply and two resistors R and S as shown in Fig. 5.2.
Fig. 5.2
The resistance of R is 25kΩ and the resistance of S is 220kΩ.
The switch can be in either position X or position Y .
The switch is in position X so that the capacitor is fully charged.
Calculate the energy E stored in the capacitor.
(energy stored =) area under line or 21 QV
=1/2×8.0×1.2×10−4=4.8×10−4 J
The switch is now moved to position Y.
Show that the time constant of the discharge circuit is 3.3 s .
(t=) R C
( t= ) 220×103×(1.2×10−4/8.0)=3.3 s
The fully charged capacitor in (a) stores energy E.
Determine the time t taken for the stored energy to decrease from E to E / 9.
E∝V2
(so time to) Vo/3V=V0e−t/RC3Vo=Voe−t/3.331=e−t/3.3t=3.6 s
A second identical capacitor is connected in parallel with the first capacitor.
State and explain the change, if any, to the time constant of the discharge circuit.
(total) capacitance is doubled
time constant is doubled
Fig. 6.1 shows a capacitor of capacitance C connected in series with a resistor of resistance R.
Fig. 6.1
Initially the switch is open and there is a p.d. of 12 V across the capacitor.
At time t=0, the switch is closed so that there is a current I in the resistor.
Fig. 6.2 shows the variation of I with t.
Fig. 6.2
Explain the shape of the line in Fig. 6.2.
p.d. across capacitor proportional to charge on capacitor
- p.d. across capacitor = p.d. across resistor
- current in resistor proportional to p.d. across resistor
- current in resistor = rate of decrease of charge on capacitor
Any two points, 1 mark each
charge proportional to current so rate of decrease of current decreases as current decreases (therefore exponential shape)
Use Fig. 6.2 to determine:
the time constant τ of the circuit in Fig. 6.1.
correct read-off of at least one pair of values for I and t
attempted read-off of t when I=0.048 mA
or
substitution of a correct pair of values of I and t into I=0.13exp(−t/τ)τ=4.3 s
Use your answers in (b) to determine capacitance C.
τ=RCC=τ/R=4.3/(9.2×104)=4.7×10−5 F
A capacitor C is charged so that the potential difference (p.d.) V across its terminals is 8.0 V . The capacitor is connected into the circuit of Fig. 6.1.
Fig. 6.1
The switch is initially open. The switch is closed at time t=0.
Fig. 6.2 shows the variation of V with the charge Q on the plates of capacitor C as the capacitor discharges.
Fig. 6.2
Show that the energy stored in capacitor C at time t=0 is 1.8 mJ .
energy stored = area under graph
=1/2×450×10−6×8.0=1.8×10−3 J or 1.8 mJ
Determine the capacitance of capacitor C . Give a unit with your answer.
C=Q / V or E=1/2CV2C=(450×10−6)/8.0 or (2×1.8×10−3)/8.02=5.6×10−5 F
Fig. 6.3 shows the variation with t of −ln(8.0 VV).
Fig. 6.3
Show that, when t is equal to one time constant, the value of −ln(8.0 VV) is equal to 1.0 .
V=V0exp(−t/RC) and τ=RCV=V0exp(−t/τ)V0=8.0 V, and at one time constant, t=τV/8.0=exp(−τ/τ), so ln(V/8.0)=−1.0 or −ln(V/8.0)=1.0
Determine the time constant τ of the circuit in Fig. 6.1.
[ t read from graph at −ln(V/8.0)=1.0]:τ=3.2 s
Calculate the resistance of resistor R.
resistance = Ω
τ=RCR=3.2/(5.6×10−5)=5.7×104Ω