1What dimensional analysis does
Dimensional analysis means working with the dimensions of quantities, their powers of , and , instead of their numbers. It needs no experiment: only the dimensional formulas you already know. It does three jobs:
- Check whether an equation could be right.
- Derive how one quantity depends on others.
- Convert a value from one system of units to another.
2Checking equations
The principle of homogeneity says that every term of a correct equation has the same dimensions. You can only add, subtract or equate like quantities: metres to metres, never metres to seconds.
Whatever sits inside , , or must be dimensionless. In , the product has no dimensions, so .
3Deriving a formula
When you know which quantities something depends on, dimensional analysis can find how. The steps:
- List the quantities it depends on.
- Assume a product of powers, , where is a pure number.
- Write the dimensions of every quantity.
- Match the powers of M, L and T on both sides. This gives one equation for each.
- Solve for , , and write the formula, keeping .
4Finding the dimensions of constants
When a formula contains unknown constants, homogeneity fixes their dimensions: each term must have the dimensions of the whole.
Some groups of quantities have no dimensions at all. The Reynolds number tells smooth flow from swirling flow, and is the same pure number in any unit system:
5Converting units
A quantity is the same whatever units you use, so : a bigger unit needs a smaller number. For a quantity with dimensions :
6What it cannot do
- It cannot find pure numbers such as , or .
- It cannot derive a formula that is a sum of terms, such as or . It only finds a single product of powers.
- It cannot make trigonometric, logarithmic or exponential functions, as in or .
- In mechanics, M, L and T give only three equations, so it can find at most three unknown powers. If a quantity depends on four or more others, it cannot fix them all.
- It cannot tell apart quantities with the same dimensions: work and torque are both .
- A dimensionally correct equation can still be wrong by a pure number.
| Job | What it can do | What it cannot do |
|---|---|---|
| Check equations | Show that an equation is wrong | Prove that an equation is right |
| Derive formulas | Find a product of powers | Find pure numbers, sums, sin, log, eˣ |
| Find constants | Give the dimensions of a constant | Tell apart quantities with the same dimensions |
| Convert units | Move a value between unit systems | — |
7A quick plan for problems
- Checking: find the dimensions of each term separately, and check that they all match. Look inside sin, cos, log and exp: that part must be dimensionless.
- Deriving: list the quantities, assume a product of powers with a pure number , write one equation each for M, L and T, solve, and keep in the answer.
- Converting: write the dimensional formula, note the ratio of each base unit, and apply the conversion rule with the right powers.
Summary
Key ideas
- Dimensional analysis checks equations, derives formulas and converts units, using only dimensions.
- Principle of homogeneity: every term of a correct equation has the same dimensions.
- Only like quantities can be added, subtracted or equated.
- What sits inside sin, cos, log or eˣ must be dimensionless.
- A failed check proves an equation wrong; a pass only means it might be right.
- To derive a formula, assume Q = k Aᵃ Bᵇ Cᶜ and match the powers of M, L and T.
- A pendulum's period is T = k√(l/g): it does not depend on the mass of the bob.
- The unknown constant k is a pure number, found by experiment (2π for the pendulum, 6π in Stokes' law).
- Homogeneity gives the dimensions of unknown constants in a formula.
- To convert units, multiply by each base-unit ratio raised to its power in the dimensional formula.
- The method cannot find pure numbers, sums, trigonometric, log or exponential forms, or more than three unknown powers.
- Same dimensions do not mean the same quantity: work and torque are both [ML²T⁻²].
Every equation
- Homogeneity
- Check s = ut + ½at²
- Check v² = u² + 2as
- Assumed form
- Pendulum
- Stokes' law
- Centripetal force
- Speed of sound
- Liquid drop
- Spring
- Constant A in F = Av + Bv³
- Constant B in F = Av + Bv³
- Constant a in P = a/V − b/V²
- Constant b in P = a/V − b/V²
- Planck's constant
- Reynolds number
- Mass with F, L, T as base
- Conversion rule
- Dyne
- Erg
- Watt
- G in CGS