Logarithms and exponential equations
Logarithms as inverse exponentials 1.06
- Logarithm: means exactly , where the base satisfies and , and the argument satisfies .
- Natural logarithm: is shorthand for , the logarithm to base ; an unsubscripted on a calculator means .
- A logarithm is an exponent: is the power to which must be raised to give .
- and , for every valid base .
- and — the two statements that and undo one another.
- Only positive arguments have a logarithm, so is undefined for ; every solution of a logarithmic equation must therefore be checked against the original equation before it is accepted.
- The graph of is the reflection of in the line : it passes through , has the -axis as a vertical asymptote, and is defined only for .
- The base restrictions , exist for the same reason a negative or unit base makes either ambiguous or constant — inherits every restriction on the exponential it inverts.
Laws of logarithms 1.06
- Product law: .
- Quotient law: .
- Power law: , for any real .
- Reciprocal case of the power law: .
- Change of base: , obtained by taking natural logarithms of .
- Each law mirrors an index law exactly, because that is where it comes from: multiplying powers adds their exponents, and a logarithm is an exponent, so .
- There is no law for ; it does not simplify at all, and writing is one of the most heavily penalised errors in this topic.
- Likewise and are different objects — only the second one equals .
- The change-of-base formula works with any base on the right, not just — is just as valid, useful when a calculator only has a base- key.
Solving equations with an unknown exponent 1.06
- , for , and .
- When the unknown appears in exponents on both sides, as in , the same method gives and hence .
- Take logarithms of both sides of the equation, using or consistently throughout.
- Use the power law to bring each unknown exponent down as a multiplier.
- Collect the terms in the unknown on one side and factorise it out.
- Divide to make the unknown the subject, then evaluate to three significant figures unless an exact answer is requested.
- The base of the logarithm taken makes no difference to the final answer, provided the same base is used on both sides — is the usual choice.
- Taking logarithms converts a multiplicative relationship in the exponent into an additive one that ordinary linear algebra can then isolate; that is the whole reason logarithms exist.
- where is negative — carry that sign carefully through the rest of the algebra rather than treating as automatically positive.
Equations that reduce to a quadratic 1.06
- Spot the repeated block: an equation in and is a quadratic in , since ; an equation in and is a quadratic in .
- Substitute a single letter for that block, for example or .
- Solve the resulting quadratic in by factorising or the formula.
- Reverse the substitution for each root, and discard any root that is not attainable.
- for every real , so a negative or zero value of must be rejected — it yields no solution rather than an extra one.
- By contrast can take any real value, so both roots of a quadratic in normally survive; it is the resulting -values that must satisfy .
- After reversing the substitution, always re-check each candidate -value in the ORIGINAL equation, not just the substituted one — a valid can still lead to an that fails a domain condition elsewhere in the equation.
Worked examples
Worked example
Write as a single logarithm, and hence evaluate it exactly.
Show worked solution
By the power law,
By the quotient law,
Since , the value is .
Worked example
Solve , giving your answer to three significant figures.
Show worked solution
Take logarithms of both sides: , so .
Then:
(3 s.f.).
Worked example
Solve:
Show worked solution
Combine the left side with the product law:
Undo the logarithm:
so , which factorises as:
giving or .
The value makes both original logarithms undefined, so it is rejected.
Hence .
Check:
Worked example
Solve:
giving your answers to three significant figures.
Show worked solution
Since , put to get , so:
and or .
Both are positive, so both are attainable values of .
Taking natural logarithms:
(3 s.f.) or (3 s.f.).
The functions eˣ and ln x
The number e and the natural logarithm 1.06
- is defined so that the gradient of at any point equals the -value at that point — the unique base for which this is true.
- , which is exactly why exponential models in calculus are written in terms of rather than any other base.
- for , and for all real .
- , , and as .
- Any exponential can be rewritten to base : .
- The graph of passes through , is positive and increasing everywhere, and has the -axis as a horizontal asymptote as .
- The graph of is its reflection in : domain , crossing the -axis at , increasing but ever more slowly.
- is irrational, like — never round it early in a calculation; keep it as symbolically until the final numerical answer is required.
Exponential growth and decay
Exponential growth and decay models 1.06
- Exponential model: , where is the initial value of at and is the growth constant.
- gives growth and gives decay; the larger is, the faster the change.
- Differentiating the model gives : the rate of change is always proportional to the current amount, which is the defining feature of exponential behaviour.
- The model is therefore the natural choice whenever a quantity's rate of change depends on how large the quantity currently is.
- Equivalent form: describes the same family, with ; a decay model has .
- carries units of 'per unit time', so its numerical value depends on whether is measured in seconds, years or any other unit — always state the unit alongside it.
- A pure exponential decay model never reaches zero; a model with a non-zero limiting value, such as cooling towards room temperature, takes the form with .
- is read directly from the model at (since ), so it never needs solving for separately if the initial value is already known or given.
Doubling time and half-life 1.06
- Doubling time : , so .
- Half-life in the decay model : , so again.
- Time to reach a general multiple of the initial value: .
- Write the model and substitute the stated multiple of the initial value, for example for a doubling or for a half-life.
- Cancel from both sides, leaving an equation in alone.
- Take natural logarithms of both sides.
- Rearrange for whichever of or is unknown.
- Because cancels, doubling time and half-life do not depend on the starting amount at all — a striking property of exponential change that no other simple model shares.
- Be careful with signs: in the positive constant is , so a half-life gives , whereas in the same decay gives .
- After several half-lives , the remaining amount is — a quick mental-arithmetic route to an approximate answer without needing the exponential form at all.
Worked example
Worked example
A radioactive isotope decays according to .
Given that the isotope has a half-life of years, find the value of .
Show worked solution
After one half-life,
when :
so:
Taking natural logs:
so , giving:
(3 s.f.).
Modelling with exponentials
Linearising a model with logarithms 1.06
- Exponential model: gives , a straight line when is plotted against , with gradient and vertical intercept .
- Base- exponential model: gives , again a straight line of against , with gradient .
- Power model: gives , a straight line when is plotted against , with gradient and intercept .
- Decide which model is proposed, and hence whether to plot against (exponential) or against (power).
- Take the logarithms of the data values and plot the transformed points.
- Read the gradient and intercept off the line of best fit.
- Recover the parameters by reversing the logarithm, for example and for the exponential model.
- The shape of the transformed plot is itself the evidence: a straight log-linear plot supports an exponential law, while a straight log-log plot supports a power law.
- The intercept is a logarithm of the constant, not the constant itself — forgetting to exponentiate before quoting is the standard error here.
- Match the base of logarithm used in plotting to the base used when recovering the constants — using to plot but to recover (or vice versa) silently gives the wrong constant.
Worked example
Worked example
The mass grams of a chemical remaining after minutes is modelled by .
Plotting against gives a straight line of gradient passing through the vertical axis at .
Find and , and find the time at which the mass has fallen to g.
Show worked solution
Taking logarithms of the model gives , so the plotted line is:
Comparing: per minute, and , so:
(3 s.f.).
For :
so:
giving minutes (3 s.f.).
Check:
as required.
Per disputationem veritatem quaerimus