MA2 - Predicting formulae
Dimensional analysis can narrow a proposed formula to a particular combination of powers. You will equate exponents, interpret the resulting model and recognise what dimensions cannot determine about constants, functions and missing variables.
Finding powers using dimensions
If a resistance force depends only on fluid density, sphere radius and speed, what powers could appear in its formula? A full theory of fluid motion is difficult; dimensions can still constrain a proposed product of powers.
Suppose , where is dimensionless, is density, is radius and is speed. Write the dimensions first, then compare the exponents of each independent base dimension. Multiplying powers adds their exponents; .
Worked example 1: predicting a force law
Question. Find if is dimensionally consistent and is dimensionless.
Plan. Expand the dimensions and match mass, length and time powers separately.
Thus , , and . Hence and , giving .
Answer. : the candidate is .
Check. , independently recovering force dimensions.
Change only the quantity being modelled, from resistance force to the power needed to overcome it at steady speed. The extra factor of speed should change the result in a predictable way.
Worked example 2: predicting the associated power
Question. Find if power , with the same variables and dimensionless .
Plan. Use and solve the three exponent equations.
So and , giving .
Answer. .
Check. Multiplying the force candidate from example 1 by , as in , gives the same powers. Doubling speed multiplies candidate force by but candidate power by .
The algebra predicts a form only under the stated list of variables and product-of-powers assumption. It has not shown that the model describes every speed or every fluid.
Watch out
Wrong: . The power acts on the whole density dimension: . Also retain any stated dimensions of a constant.
Try another target quantity using the same building blocks.
Limits on constants and functions
A dimensional prediction cannot choose between and : both have the same dimensions. The dimensionless coefficient requires physical theory or measurements. It can vary between different shapes or conditions; it is held constant only within the chosen model.
Nor does dimensional analysis automatically establish a product of powers. Suppose a pendulum period depends on length , gravitational acceleration and release angle . Since an angle in radians is dimensionless, every expression of the form
has the dimensions of time for any dimensionless function . Dimensions cannot tell you whether is constant, or how period changes with angle. For the small-angle simple-pendulum model, theory gives the coefficient ; dimensions alone cannot supply it or establish the small-angle condition.
Inputs to , and in physical formulae must be dimensionless. For example, is meaningful when is a time. Writing as a physical law hides a timescale unless has explicitly been made dimensionless. A numerical formula using “ measured in seconds” is a different convention and must state that convention.
If two lengths and are allowed, their ratio is dimensionless. A formula may contain an unknown function of that ratio, so dimensions may leave freedom rather than determine unique powers. That is useful information about what further evidence is needed.
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