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Physics - Measurements and uncertainties

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1.1 Measurements in Physics
Standard/scientific form​ - a form of writing large numbers. Eg: 123000 = 1.23 x 10​5
Fundamental quantities: ​a unit of measurement for a measurable physical quantity from which every
other unit or quantity can be derived. ​Derived ​quantities are derived from the multiplication or division
of one fundamental quantity with another.
Base quantity
Unit
Symbol
Length
meter
m
Mass
kilogram
kg
Time
seconds
s
Electric current
amperes
A
Thermodynamic temperature
kelvin
K
Amount of substance
moles
mol.
Orders of magnitude
These are numbers on a scale where each number is rounded to the nearest power of 10.
For eg: 2000m = 2 x 10​3​ ⇒ 10​3​ (when the number is less than 5, just the power is taken)
: 5000m = 5 x 10​3​ ⇒ 10 x 10 3​​ = 10​4​ (when greater than or equal to 5, estimate to 10)
Orders of magnitude to memorize
Diameter of proton/nucleus = 10​-15​ m
Diameter of atom = 10​-10​m
Diameter of the universe = 10​25​m
Mass of an electron = 9.11 x 10​-31​kg ⇒ 10 x 10​-31​ = 10​-30
Mass of the universe = 10​50
Time it takes light to travel across a nucleus = s/v = 10​-15​/10​8​ (from 3 x 10​8​) = 10​-23​s
Age of the universe = 10​17​ s
Also know how to use metric multipliers (eg: kilo, mega, deca, deci, centi, etc.), compare ratios, values,
and approximations, and estimate significant figures as appropriate.
Significant figures
● A non-zero digit will always be significant (eg: 345 has 3.s.f)
● Zeros that occur between non-zero digits are always significant (eg: 303 has 3.s.f)
● Non-sandwiched zeros to the left of a non-zero digit are not significant (eg: 0.34 is 2.s.f)
● Zeros that occur to the right of a decimal point are significant (eg: 1.00 is 3.s.f.)
● When there is no decimal point, trailing zeros are not significant (eg: 400 is 1.s.f)
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1.2 Uncertainties and errors
If the same thing is measured
repeatedly, and you get the same
value, then the result is ​precise​. If the
measured value is close to the expected
value, then the result is a​ ccurate
Types of error
Random error​ - random fluctuations in the measured data. This is caused due to​:
● Poor readability of the instrument
● The effects of changes in the surroundings
● The carelessness of the experimenter
Precise experiments have small random errors. To reduce random error, take more repeats, and
average​.
Systematic error​ - occur when there is something wrong with the method or the equipment. For eg:
● Zero error​ - When the zero setting of a piece of apparatus shifts after constant usage,
● Meter ruler edges are chipped/rounded
● Improper calibration
Accurate experiments have a small systematic error. To reduce, use instruments of higher quality
Absolute uncertainty in measurement
Two ways of calculation (larger value is taken as the uncertainty):
Option 1:
(maximum measurement - minimum measurement)/2
Option 2:
Take the arithmetic mean of the measurements, and the mean is considered to be the literature value.
The greatest deviation of any of the measurements is taken as the uncertainty.
Absolute and Fractional uncertainties
Uncertainties in the form of ​±Δ
​ x are known as ​absolute uncertainties. ​These values have the same unit as
the quantity and should have the same s.f. Suppose the diameter of a ball is 10cm, and there is an
absolute uncertainty of 1cm. Dividing the absolute uncertainty by the value itself gives us a
dimensionless value known as the ​fractional uncertainty​. The fractional uncertainty would be written as
1/10 = 0.1 (10% as a ​percentage of the uncertainty​).
Uncertainty in equipment
For an ​analog scale, the ​uncertainty is ± half of the smallest scale division. For a ​digital ​scale, the
uncertainty​ is ± 1 in the least significant digit
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Propagation of uncertainties ------------------------------------------->
Significant figures in calculations
● Addition and subtraction
○ When values are added or subtracted, the number of
decimal places on the least precise data determines the
precision of the calculated value.
●
Multiplication and division
○ Whenever you multiply or divide data, the answer should
be quoted to the same number of significant figures as the least precise data
Drawing graphs
Error bars
The table below compares the masses of plasticine balls of different diameters.
Since we have just 4 data points, there is not enough
distribution to use the standard deviation formula. Instead we:
Even though the uncertainty is exaggerated, this calculation is
accepted for smaller calculations.
The uncertainties can be represented using error bars on a graph.
For easier analysis, this model has to be ​linearized​:
⍴ = mass/volume
Volume = (4𝜋r​3​)/3
∴ ⍴ = 3m/4𝜋r​3
When rearranged: r​3​ = 3m/4𝜋⍴
r = d/2, so r​3​ = d​3​/8 = 3m/4𝜋⍴
d​3​ = 6m/𝜋⍴
6/𝜋⍴ is a constant, so d​3 must be proportional to m. Using an extension of the initial table, a linearized
model can now be plotted. The length of the error bar in either direction represents the uncertainty.
As per the formula, d​3 is directly
proportional to m. But the line does not pass
through the origin. This is due to ​systematic
error
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Uncertainty in the gradient
From the equation d​3​ = 6m/𝜋⍴, we know that the gradient of the line is 6/𝜋⍴ (y = mx+c).
By calculation, the gradient of the line should be 1.797.
1.797 = 6/𝜋⍴, So ⍴ = 6/1.797𝜋 = 1.063 g/cm​3
To find the uncertainty we draw the steepest and the least steep lines through the error bars:
This gives the steepest grad. = 1.856 cm​3​/g and least steep
grad. = 1.746 cm​3​/g. So uncertainty in the gradient using the
smaller sample formula gives:
(1.856 - 1.746)/2 = 0.06cm​3​/g
If we enter the max and min values of the gradient, we obtain a max and min density:
⍴​max​ = 6/1.746𝜋 = 1.09 and ⍴​min​ = 6/1.856𝜋 = 1.03
Therefore the density can be written as 1.06 ​±​ 0.03 g/cm​3
Relationships (for data recording) ​(Think about uncertainty propagation when linearizing)
Linearisation by manipulating the axis
Linearisation using logs
Linear
Non-linear
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1.3 Vectors and Scalars
A v​ ector​ is a quantity with both direction and magnitude
Vector Addition
Vectors can be represented using arrows. The length of the arrow is proportional
to the magnitude of the vector, and the arrowhead indicates the direction of the
vector. To add vectors, the arrows are placed from tip to tail, to give a r​ esultant​.
Basic trigonometry (applies to most vector problems)
These equations only apply to right-angled triangles. The hypotenuse is
the longest side of the triangle. The three sides of a triangle are connected
by the ​Pythagoras theorem:
Hypotenuse​2​ = Opposite​2​ + Adjacent​2
For ​vectors in 1D​, there is only forward and backward, so the magnitudes
of the vectors are added to give a resultant. If +ve, the resultant direction
is forward and vice versa.
Subtracting vectors
A negative vector is in an opposite direction to a positive vector.
Hence, to subtract a vector, you just add the vector with the
negative magnitude to the other vector.
Scalar​ quantities have magnitude but no direction.
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