Physics ERROR IN MEASUREMENT

Error in Measurement

In general, the errors in measurement can be broadly classified as
(a) systematic errors and
(b) random errors.

`text(Systematic errors :)`
The systematic errors are those errors that tend to be in one direction, either positive or negative. Some of the sources of systematic errors are :

(a) `text(Instrumental errors)` that arise from the errors due to imperfect design or calibration of the measuring instrument, zero error in
the instrument, etc. For example, the temperature graduations of a thermometer may be inadequately calibrated (it may read 104 -C at the boiling point of water at STP whereas it should read 100 -C); in a vernier callipers the zero mark of vernier scale may not coincide with the zero mark of the main scale, or simply an ordinary metre scale may be worn off at one end.

(b) `text(Imperfection in experimental technique or procedure)` To determine the temperature of a human body, a thermometer placed under the armpit will always give a temperature lower than the actual value of the body temperature. Other external conditions (such as changes in temperature, humidity, wind velocity, etc.) during the experiment may systematically affect the measurement.

(c) `text(Personal errors)` that arise due to an individual-s bias, lack of proper setting of the apparatus or individual-s carelessness in taking observations without observing proper precautions, etc. For example, if you, by habit, always hold your head a bit too far to the right while reading the position of a needle on the scale, you will introduce an error due to parallax.

Systematic errors can be minimised by improving experimental techniques, selecting better instruments and removing personal bias as far as possible.

`text(Random errors :)`
The random errors are those errors, which occur irregularly and hence are random with respect to sign and size. These can arise due to random and unpredictable fluctuations in experimental conditions (e.g. unpredictable fluctuations in temperature, voltage supply, mechanical vibrations of experimental set-ups, etc), personal (unbiased) errors by the observer taking readings, etc. For example, when the same person repeats the same observation, it is very likely that he may get different readings everytime.

`text(Least count error :)`
The least count error is the error associated with the resolution of the instrument. For example, a vernier callipers has the least count as 0.01 cm; a spherometer may have a least count of 0.001 cm. Least count error belongs to the category of random errors but within a limited size; it occurs with both systematic and random errors.

Absolute Error, Relative Error and Percentage Error

`text(Absolute Error :)`
The magnitude of the difference between the true value of the quantity and the individual measurement value is called the absolute error of the measurement.

This is denoted by `| Δa |`.

In absence of any other method of knowing true value, we considered arithmetic mean as the true value.

Suppose the values obtained in several measurements are `a_1, a_2, a_3...., a_n`. The arithmetic mean of these values is taken as the best possible value of the quantity under the given conditions of measurement as :

`a_(mean) = (a_1+a_2+a_3+...+a_n ) / n`

`a_(mean) = sum_(t=1)^na_t//n`

The errors in the individual measurement values are

`Δa_1 = a_(mean) - a_1`,
`Δa_2 = a_(mean) - a_2`,
`.... .... ....`
`.... .... ....`
`Δa_n = a_(mean) - a_n`.

The `Δa` calculated above may be positive in certain cases and negative in some other cases. But absolute error `|Δa|` will always be positive.

The arithmetic mean of all the absolute errors is taken as the final or mean absolute error of the value of the physical quantity a. It is represented by `Δa_(mean)`.

Thus,

`Δa_(mean) = (|Δa_1|+|Δa_2 |+|Δa_3|+...+ |Δa_n|)/n`

`Deltaa_(mean) = sum_(t=1)^n|Deltaa_t|//n`

If we do a single measurement, the value we get may be in the range `a_(mean) - Δa_(mean)`

`text(Relative and Percentage Error :)`
we often use the relative error or the percentage error (`δa`). The relative error is the ratio of the mean absolute error `Δa_(mean)` to the mean value `a_(mean)` of the quantity measured.

`text(Relative error)` `= (Δa_(mean))/a_(mean)`

When the relative error is expressed in percent, it is called the percentage error (`δa`).

Thus, Percentage error `δa = (Δa_(mean))/(a_(mean)) - 100%`

`text(Combination of Errors :)`
If we do an experiment involving several measurements, we must know how the errors in all the measurements combine.

(a) `text(Error of a sum or a difference)` Suppose two physical quantities A and B have measured values `A - ΔA`, `B - ΔB` respectively where `ΔA` and `ΔB` are their absolute errors. We wish to find the error `ΔZ` in the sum

`Z = A + B`.

We have by addition, `Z - ΔZ = (A - ΔA) + (B - ΔB)`.

The maximum possible error in Z

`ΔZ = ΔA + ΔB`

For the difference `Z = A - B`,

we have `Z - Δ Z = (A - ΔA) - (B - ΔB)`

`= (A - B) - ΔA - ΔB`
or, `- ΔZ = - ΔA - ΔB`

The maximum value of the error `ΔZ` is again `ΔA + ΔB`.

`text(When two quantities are added or subtracted, the absolute error in the final result is the sum of the absolute errors in the individual quantities)`.

(b) `text(Error of a product or a quotient)` Suppose `Z = AB` and the measured values of A and B are A - ΔA and B - ΔB.

Then `Z - ΔZ = (A - ΔA) (B - ΔB)`
`= AB - B ΔA - A ΔB - ΔA ΔB`

Dividing LHS by Z and RHS by AB we have,
`1-((ΔZ)/Z) = 1 - ((ΔA)/A) - ((ΔB)/B) - ((ΔA)/A)((ΔB)/B)`.

Since `ΔA` and `ΔB` are small, we shall ignore their product.

Hence the maximum relative error
`(ΔZ)/ Z = ((ΔA)/A) + ((ΔB)/B)`

`text(When two quantities are multiplied or divided, the relative error in the result is the sum of the relative errors in the multipliers.)`

(c) `text(Error in case of a measured quantity raised to a power)` Suppose `Z = A^2`,

Then,
`(ΔZ)/Z = ((ΔA)/A) + ((ΔA)/A) = 2 ((ΔA)/A)`

Hence, the relative error in `A^2` is two times the error in A.

In general, if `Z = A^p B^q//C^r`

Then,
`(ΔZ)/Z = p ((ΔA)/A) + q ((ΔB)/B) + r ((ΔC)/C)`

`text(The relative error in a physical quantity raised to the power k is the k times the relative error in the individual quantity.)`

 
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