Chapter overview
Physics studies measurable quantities. A physical quantity is expressed as:
Physical quantity=numerical value×unit
Example:
l=5 m
Here, 5 is the numerical value and m is the unit.
1. Fundamental and derived quantities
Fundamental quantities are independent quantities. Derived quantities are obtained from fundamental quantities.
| Quantity | SI unit | Symbol |
|---|
| Length | metre | m |
| Mass | kilogram | kg |
| Time | second | s |
| Electric current | ampere | A |
| Temperature | kelvin | K |
| Amount of substance | mole | mol |
| Luminous intensity | candela | cd |
2. Derived units
| Quantity | Formula | SI unit |
|---|
| Area | l2 | m2 |
| Volume | l3 | m3 |
| Velocity | timedisplacement | m s−1 |
| Acceleration | timevelocity | m s−2 |
| Force | ma | kg m s−2 or N |
| Work | Fs | kg m2s−2 or J |
| Power | tW | kg m2s−3 or W |
3. Dimensions
Dimensions represent the powers of fundamental quantities in a physical quantity.
| Quantity | Dimensional formula |
|---|
| Length | [L] |
| Mass | [M] |
| Time | [T] |
| Velocity | [LT−1] |
| Acceleration | [LT−2] |
| Force | [MLT−2] |
| Work/Energy | [ML2T−2] |
| Power | [ML2T−3] |
| Pressure | [ML−1T−2] |
Example:
F=ma
Dimensional formula:
[F]=[M][LT−2]=[MLT−2]
4. Dimensional analysis
Principle of homogeneity
Only physical quantities with the same dimensions can be added or subtracted.
If:
A+B=C
then:
[A]=[B]=[C]
Example:
s=ut+21at2
Checking dimensions:
[ut]=[LT−1][T]=[L]
[at2]=[LT−2][T2]=[L]
So the equation is dimensionally correct.
5. Uses of dimensional analysis
To check correctness of equations
Example:
T=2πgl
Dimension of RHS:
[gl]=[LT−2][L]=[T2]=[T]
So the formula is dimensionally correct.
To derive relations
Suppose time period of a simple pendulum depends on length l and acceleration due to gravity g.
T∝lagb
So:
[T]=[L]a[LT−2]b
[T]=[La+bT−2b]
Equating powers:
a+b=0,−2b=1
Therefore:
b=−21,a=21
Hence:
T∝gl
6. Limitations of dimensional analysis
- It cannot determine dimensionless constants like 2, π, or 21.
- It cannot distinguish between scalar and vector quantities.
- It cannot derive equations involving trigonometric, exponential, or logarithmic functions.
- It cannot verify equations where dimensions are correct but physics is wrong.
7. Significant figures
Significant figures are meaningful digits in a measured quantity.
Examples:
| Number | Significant figures |
|---|
| 2.34 | 3 |
| 0.0045 | 2 |
| 5.060 | 4 |
| 100.0 | 4 |
Rules:
- All non-zero digits are significant.
- Zeros between non-zero digits are significant.
- Leading zeros are not significant.
- Trailing zeros after decimal are significant.
8. Accuracy and precision
Accuracy means closeness to the true value.
Precision means closeness among repeated measurements.
9. Errors in measurement
Measured value:
a1,a2,a3,…,an
Mean value:
aˉ=na1+a2+⋯+an
Absolute error:
Δai=∣ai−aˉ∣
Mean absolute error:
Δamean=nΔa1+Δa2+⋯+Δan
Relative error:
aΔa
Percentage error:
aΔa×100
10. Combination of errors
Addition and subtraction
If:
Z=A+B
or:
Z=A−B
then:
ΔZ=ΔA+ΔB
Multiplication and division
If:
Z=AB
or:
Z=BA
then:
ZΔZ=AΔA+BΔB
Powers
If:
Z=An
then:
ZΔZ=nAΔA
General rule:
Z=ApBqCr
then:
ZΔZ=pAΔA+qBΔB+rCΔC
11. Vernier calipers and screw gauge
Least count of vernier calipers:
LC=number of divisions on vernier scale1 MSD
Measurement:
Reading=main scale reading+vernier coincidence×LC
Screw gauge least count:
LC=number of circular scale divisionspitch
Screw gauge reading:
Reading=pitch scale reading+circular scale reading×LC
12. Solved examples
Example 1
Check the dimensions of:
v=u+at
Solution:
[v]=[LT−1]
[u]=[LT−1]
[at]=[LT−2][T]=[LT−1]
All terms have the same dimension, so the equation is dimensionally correct.
Example 2
If:
l=2.0±0.1 m
and:
b=3.0±0.2 m
then area:
A=lb
Relative error:
AΔA=2.00.1+3.00.2
13. Common mistakes
- Confusing units and dimensions.
- Writing SI symbols in plural form, like mts instead of m.
- Ignoring significant zeros after decimal.
- Adding percentage errors for addition/subtraction problems.
- Forgetting that dimensional analysis cannot determine constants.
14. Quick revision
| Concept | Formula |
|---|
| Force dimension | [MLT−2] |
| Work dimension | [ML2T−2] |
| Power dimension | [ML2T−3] |
| Mean | aˉ=n∑ai |
| Relative error | aΔa |
| Percentage error | aΔa×100 |
| Product error | ZΔZ=AΔA+BΔB |
| Power error | ZΔZ=nAΔA |