SI units are the basis of physics.
Physical properties have standard measurement units.
In physics we use a system known as SI units.
The basic SI units are kilograms (kg), metres (m), seconds (s), and Coulomb (C).
Physics equations all work correctly (give the right answers) if we use these units.
This makes things much easier, as there is no need to convert to other units.
We know that both sides of an equation must have exactly the same units.
This is useful because we can use this to check that the equations are correct and that the units we are using will give the right answers.
We can also use these ideas to create or guess how an equation might look.
If there are two or more terms on one side, e.g. s = vt + ½at2, then vt and ½at2 (and s) should all have the same units (in this case, metres).
Dimensions simplify this further - we don’t even need to specify whether we’re measuring kg or g or lbs or oz - if we see mass on one side of an equation we know there must be mass on the other side.
We just need to look at each side of the equation and check how many M, L, T and Q there are (where M is Mass, L is Length, T is Time, and Q is Charge).
For example: Energy is ML2/T2 , and mc2 is M(L/T)2 = ML2/T2 , so E = mc2 is a valid equation.
The equation is balanced with the correct numbers and positions of M’s, L’s, and T's on both sides.
An equation is only valid if both sides have the same M's, L's, and T's.
Balancing the units and/or dimensions is a good check to do when we see an unfamiliar equation.
Dimensions are usually taught at advanced level, but it's useful to know that this system is behind all physics relationships.
Each parameter has its own table, like the one here ------>>
The table shows the typical symbols and the SI units of the parameter.
It also gives the longform units, in terms of basic kg, m, s, and C.
The dimensions are also given - in terms of M, L, T, and Q.
These are then listed as an MLTQ code at the bottom of the table.
Lets take the example of E = mc2
The terms on the right hand side are mass x speed x speed.
When terms are multipled we can add up all their MLTQ codes.
The total MLTQ codes on both sides match.
So we prove that E = Amv2 is a valid equation, where A is a constant, such as 1 or ½.
Examples are: E = ½mv2 and E = mc2
Or if we want to find what could be the missing term X in E = mX, we can work this out by re-organising the equation, and writing X = E/m.
When terms are divided, we subtract the MLTQ code of terms on the bottom from the MLTQ code of those on the top.
So, we substract the MLTQ code of m from that of E.
This tells us that the MLTQ code of X is the same as speed2 .
So we know that E = Amv2, where A is a constant, is a possible answer.
The terms on the right hand side are multiplied so they can be added together:
In the case below, the terms on the right hand side are E/m so the MLTQ code of m is subtracted from E: