Exponential Equations: e, ln and Straight-Line Graphs - OCR A Level Physics
Module 6 - capacitors, nuclear physics and medical imaging

Exponential Equations: using e, ln and straight-line graphs

Exponential equations look different in capacitors, radioactive decay and imaging attenuation, but the same idea keeps appearing: a quantity changes by a fixed fraction in each equal step. Natural logs turn that curve into a line.

Work through it in three passes

1

Understand the shape

Learn why the original physics graph is curved and why taking ln makes a straight line.

2

Choose the right plot

Match each Module 6 equation to the graph you should draw, including background correction and capacitor charging.

3

Do the graph task

Calculate logged values, plot them, check the best-fit line, then use the gradient to find the physics constant.

By the end you should be able to

What an exponential equation is really saying

A Level Physics exponentials usually describe a quantity that changes at a rate proportional to how much of it is left. That is why the graph is curved: the value changes quickly at first, then more slowly as the value gets smaller.

Decay form

y = Ae-kx

Used when a quantity falls towards zero: capacitor discharge, radioactive activity, photon intensity through an absorber.

Approach-to-final form

y = yfinal(1 - e-kx)

Used when a quantity rises towards a maximum: capacitor voltage while charging.

The exponent must be dimensionless

In e-t/RC, the quantity t/RC has no unit because RC is a time constant in seconds. In e-λt, λ has unit s-1, so λt has no unit.

The rules you actually use

ln means natural logarithm. It is the inverse of ex, so it is the operation that "undoes" an exponential.

ln(ex) = x so ln(e-λt) = -λt
ln(ab) = ln(a) + ln(b) so ln(Ae-kx) = ln(A) - kx
ln(a/b) = ln(a) - ln(b) so ln(y/A) = -kx
eln(a) = a so if ln(A) = 2.48, then A = e2.48

Half left

e-kx = 1/2

kx = ln(2)

37% left

e-1 = 0.368

After one time constant, a decaying quantity is about 37% of its initial value.

63% reached

1 - e-1 = 0.632

After one time constant, a charging capacitor has reached about 63% of its final voltage.

Turning an exponential curve into a straight line

The straight-line equation is y = mx + c. Your job is to make an exponential look like that. For a simple decay equation:

y = Ae-kx
ln(y) = ln(A) - kx

This means if you plot ln(y) on the vertical axis against x on the horizontal axis, the graph should be a straight line with gradient -k and intercept ln(A).

Original graph: curved decay

x y

Linearised graph: straight line

x ln(y) gradient = -k
1
Rearrange first. If there is a background or final value, subtract it before taking logs.
2
Take natural logs. Use ln, not log10, because OCR exponential formulae use e.
3
Plot the transformed variable. The horizontal axis stays as time, thickness or distance; the vertical axis becomes a natural log.
4
Use the line. The gradient gives the physical constant; the intercept gives the initial value after applying eintercept.
About units inside ln

Strictly, logs are taken of dimensionless ratios, such as ln(V / 1 V) or ln(A / 1 Bq). In exam tables you will often see ln(V) for the logged numerical value. The gradient is unchanged, so the physics result is unchanged.

Where this appears in Module 6

Capacitor discharge

V = V0e-t/RC

Plot ln(V) against t. Gradient = -1/RC, so RC = -1/gradient.

Capacitor charging

VC = E(1 - e-t/RC)

Rearrange to E - VC = Ee-t/RC. Plot ln(E - VC) against t.

Radioactive decay

A = A0e-λt

Plot ln(A) against t. Gradient = -λ. Half-life T1/2 = ln(2)/λ.

Count rate with background

C = Cbg + C0e-λt

Subtract background first. Plot ln(C - Cbg) against t.

X-ray or gamma attenuation

I = I0e-μx

Plot ln(I) against x. Gradient = -μ. Or plot ln(I0/I) against x for gradient .

Medical tracers and PET

A = A0e-λt

Radiopharmaceutical activity decays exponentially. The same graphing method helps find activity, decay constant or effective half-life.

Plot the graph yourself, then check it

Your task

A capacitor is discharged through a resistor. Use the data to test whether the discharge is exponential. Calculate ln(V), plot ln(V) against t, then use the straight-line graph to find RC.

  1. Fill in the missing ln(V) values to 3 decimal places.
  2. Press Plot my points to see your transformed graph.
  3. Press Show expected graph only after you have tried.
  4. Use the gradient to calculate RC and use the intercept to find V0.

What success looks like

  • Your plotted points should lie close to a straight decreasing line.
  • The gradient should be about -0.025 s-1.
  • The time constant should be about 40 s.
  • The intercept should give an initial voltage of about 12 V.
t / sV / VYour ln(V)
012.00
207.28
404.41
602.68
801.62
time, t / s ln(V) 0 20 40 60 80 2.5 2.0 1.5 1.0
Reveal full answer and marking guide
t / sV / Vln(V)
012.002.485
207.281.985
404.411.484
602.680.986
801.620.482

gradient = (0.482 - 2.485) / (80 - 0) = -0.0250 s-1

For V = V0e-t/RC, gradient = -1/RC, so RC = -1 / -0.0250 = 40 s.

intercept = ln(V0) = 2.485, so V0 = e2.485 = 12.0 V.

Worked examples with graph choices

Example 1: capacitor discharge

A 12.0 V capacitor discharge gives the data below. Show how to find the time constant.

t / sV / Vln(V)
012.02.485
207.281.985
404.411.484
602.680.986
801.620.482

Plot ln(V) against t. The gradient is about:

gradient = (0.482 - 2.485) / (80 - 0) = -0.0250 s-1

For discharge, gradient = -1/RC.

RC = -1 / gradient = -1 / -0.0250 = 40 s

The intercept is ln(V0) = 2.485, so V0 = e2.485 = 12.0 V.

Example 2: capacitor charging needs rearranging

A capacitor charges from a 6.0 V supply. You cannot plot ln(VC) against time and expect a straight line.

Start with the charging equation:

VC = E(1 - e-t/RC)

Rearrange so the exponential is on its own:

E - VC = Ee-t/RC
ln(E - VC) = ln(E) - t/RC
t / sVC / VE - VC / Vln(E - VC)
00.006.001.792
101.984.021.391
203.302.700.993
304.191.810.593
404.791.210.191
gradient = (0.191 - 1.792) / 40 = -0.0400 s-1, so RC = 25 s

Example 3: nuclear count rate with background

A radioactive source is measured with a background count rate of 18 counts s-1.

t / sMeasured C / counts s-1Corrected C - Cbgln(C - Cbg)
02382205.394
751741565.049
1501281104.700
22596784.357
30073554.007

Plot ln(C - Cbg) against t. Do not log the uncorrected measured count rate.

gradient = (4.007 - 5.394) / 300 = -0.00462 s-1
λ = 0.00462 s-1, so T1/2 = ln(2) / λ = 0.693 / 0.00462 = 150 s

Example 4: attenuation in medical imaging

For X-ray or gamma photons through tissue, intensity often follows I = I0e-μx.

x / cmI / % of incident intensityln(I / I0)
01000.000
269.8-0.360
448.7-0.720
634.0-1.079

Plot ln(I/I0) against x. The line passes through the origin because ln(1) = 0.

gradient = -0.180 cm-1, so μ = 0.180 cm-1
half-value thickness = ln(2) / μ = 0.693 / 0.180 = 3.85 cm

This is the same mathematics as radioactive decay: distance through material replaces time, and attenuation coefficient replaces decay constant.

Common mistakes and quick fixes

Logging before rearranging

For charging capacitors, ln(VC) is not linear. Use ln(E - VC).

Forgetting background

For radioactivity, subtract background count rate before taking logs. Otherwise the graph curves and the half-life is wrong.

Losing the minus sign

If the quantity decays, the gradient is negative. The physical constant RC, λ or μ is positive.

Using two rounded points badly

Use a best-fit line over the full plotted range. Two rounded table values can shift the gradient noticeably.

Self-check questions

1. A graph of ln(V) against t for a discharging capacitor has gradient -0.0125 s-1. Find RC.

gradient = -1/RC, so RC = -1 / -0.0125 = 80 s.

2. Which graph should you plot for VC = E(1 - e-t/RC)?

Plot ln(E - VC) against t. The gradient is -1/RC.

3. A corrected count rate halves every 4.0 hours. What is the decay constant?

λ = ln(2) / T1/2 = 0.693 / 4.0 = 0.173 h-1.

4. Intensity follows I = I0e-μx. What does the gradient of ln(I/I0) against x equal?

The gradient is -μ. If you plot ln(I0/I) against x instead, the gradient is +μ.

Final checklist for graphing exponentials