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Capacitor Discharge Equations (CIE A Level Physics)

Revision Note

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Ann H

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Ann H

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Physics

The Time Constant

  • The time constant of a capacitor discharging through a resistor is a measure of how long it takes for the capacitor to discharge
  • The definition of the time constant is:

The time taken for the charge, current or voltage of a discharging capacitor to decrease to 37% of its original value

  • This is represented by the Greek letter tau (tau) and measured in units of seconds (s)
    • It is an easy way to compare the rate of change of similar quantities e.g. charge, current and p.d.
  • The time constant is defined by the equation:

τ{"language":"en","fontFamily":"Times New Roman","fontSize":"18"} = RC

  • Where:
    • τ{"language":"en","fontFamily":"Times New Roman","fontSize":"18"} = time constant (s)
    • R = resistance of the resistor (Ω)
    • C = capacitance of the capacitor (F)

  • For example, to find the time constant from a voltage-time graph, calculate 0.37V0 and determine the corresponding time for that value

 

The Time Constant on Discharging Potential Difference-Time Graphs

19-3-2-time-constant-on-graph--cie-new

The time constant shown on a discharging capacitor for potential difference

Worked example

A capacitor of 7 nF is discharged through a resistor of resistance R. The time constant of the discharge is 5.6 × 10-3 s.

Calculate the value of R.

 

Answer:

 

Step 1: Write out the known quantities

Capacitance, C = 7 nF = 7 × 10-9 F

Time constant, tau = 5.6 × 10-3 s

 

Step 2: Write down the time constant equation

tau = RC

 

Step 3: Rearrange for resistance R

bold italic R bold space bold equals bold space bold tau over bold C

 

Step 4: Substitute in values and calculate R

 

bold italic R bold space bold equals bold space fraction numerator bold 5 bold. bold 6 bold space bold cross times bold space bold 10 to the power of bold minus bold 3 end exponent over denominator bold 7 bold space bold cross times bold space bold 10 to the power of bold minus bold 9 end exponent end fraction bold space bold equals bold space bold 8 bold space bold cross times bold space bold 10 to the power of bold 5 bold space bold capital omega bold space bold equals bold space bold 800 bold space straight k straight capital omega

Using the Capacitor Discharge Equation

  • The time constant is used in the exponential decay equations for the current, charge or potential difference (p.d.) for a capacitor discharging through a resistor
    • These can be used to determine the amount of current, charge or p.d. left after a certain amount of time when a capacitor is discharging

  • All capacitor discharge equations are of the form: 

bold italic X bold space bold equals bold space bold italic X subscript bold 0 bold italic e to the power of bold minus stretchy left parenthesis fraction numerator t over denominator R C end fraction stretchy right parenthesis end exponent

  • Where:
    • = current, charge or potential difference
    • X0 = initial current, charge or potential difference before discharge
    • e = the exponential function
    • t = time (s)
    • RC = resistance (Ω) × capacitance (F) = the time constant tau (s)

 

  • This equation shows that the faster the time constant tau, the quicker the exponential decay of the current, charge or p.d. when discharging
  • Also, how big the initial current, charge or p.d. is affects the rate of discharge
    • If X0 is large, the capacitor will take longer to discharge

  • Note: during capacitor discharge, X0 is always larger than X, this is because the current, charge or p.d. will always be decreasing
  • The current at any time is directly proportional to the p.d across the capacitor and the charge across the parallel plates
  • The exponential decay of current on a discharging capacitor is defined by the equation:

bold italic I bold space bold equals bold space bold italic I subscript bold 0 bold italic e to the power of stretchy left parenthesis negative t over RC stretchy right parenthesis end exponent

  • Where:
    • I = current (A)
    • I0 = initial current before discharge (A)

  • The equation for exponential decay of charge on a discharging capacitor is defined by the equation:

bold italic Q bold space bold equals bold space bold italic Q subscript bold 0 bold italic e to the power of stretchy left parenthesis negative fraction numerator t over denominator R C end fraction stretchy right parenthesis end exponent

  • Where:
    • Q = charge on the capacitor plates (C)
    • Q0 = initial charge on the capacitor plates (C)

  • The equation for exponential decay of p.d. on a discharging capacitor is defined by the equation:

bold italic V bold space bold equals bold space bold italic V subscript bold 0 bold italic e to the power of stretchy left parenthesis negative fraction numerator t over denominator R C end fraction stretchy right parenthesis end exponent

  • Where:
    • V = potential difference on the capacitor plates (V)
    • V0 = initial potential difference on the capacitor plates (V)

The Exponential Function, e

  • The symbol e represents the exponential constant, a number which is approximately equal to e = 2.718...
  • On a calculator, it is shown by the button ex
  • The inverse function of ex is ln(y), known as the natural logarithmic function
    • This is because, if ex = y, then x = ln(y)

  • The 0.37 in the definition of the time constant arises as a result of the exponential constant, the true definition is:

The time taken for the charge of a capacitor to decrease to bold 1 over bold e of its original value

  • Where 1 over e = 0.3578

Worked example

The initial current through a circuit with a capacitor of 620 μF is 0.6 A. The capacitor is connected across the terminals of a 450 Ω resistor.

Calculate the time taken for the current to fall to 0.4 A.

 

Answer: 

 

Step 1: Write out the known quantities

Initial current before discharge, I0 = 0.6 A

Current, I = 0.4 A

Resistance, R = 450 Ω

Capacitance, C = 620 μF = 620 × 10-6 F

Step 2: Write down the equation for the exponential decay of current

 

bold italic I bold space bold equals bold space bold italic I subscript bold 0 bold italic e to the power of stretchy left parenthesis negative t over RC stretchy right parenthesis end exponent

 

Step 3: Calculate the time constant

tau = RC

tau = 450 × (620 × 10-6) = 0.279 s

Step 4: Substitute into the current equation

bold 0 bold. bold 4 bold space bold equals bold space bold 0 bold. bold 6 bold space bold cross times bold space bold italic e to the power of bold minus fraction numerator bold t over denominator bold 0 bold. bold 279 end fraction end exponent

Step 5: Rearrange for the time t

fraction numerator bold 0 bold. bold 4 over denominator bold 0 bold. bold 6 end fraction bold space bold equals bold space bold italic e to the power of bold minus fraction numerator bold t over denominator bold 0 bold. bold 279 end fraction end exponent

      The exponential can be removed by taking the natural log of both sides:

bold italic l bold italic n stretchy left parenthesis fraction numerator 0.4 over denominator 0.6 end fraction stretchy right parenthesis bold space bold equals bold space bold minus fraction numerator bold t over denominator bold 0 bold. bold 279 end fraction

 

bold italic t bold space bold equals bold space bold minus bold 0 bold. bold 279 bold space bold cross times bold space bold italic l bold italic n stretchy left parenthesis fraction numerator 0.4 over denominator 0.6 end fraction stretchy right parenthesis bold space bold equals bold space bold 0 bold. bold 1131 bold space bold equals bold space bold 0 bold. bold 1 bold space bold italic s

Exam Tip

Make sure you’re confident in rearranging equations with natural logs (ln) and the exponential function (e). To refresh your knowledge of this, have a look at the AS Maths revision notes on Exponentials & Logarithms

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Ann H

Author: Ann H

Ann obtained her Maths and Physics degree from the University of Bath before completing her PGCE in Science and Maths teaching. She spent ten years teaching Maths and Physics to wonderful students from all around the world whilst living in China, Ethiopia and Nepal. Now based in beautiful Devon she is thrilled to be creating awesome Physics resources to make Physics more accessible and understandable for all students no matter their schooling or background.