11th Class

The measuring process is essentially a process of comparison. Inspite of our best efforts, the measured value of a quantity is always somewhat different from its actual value, or true value. This difference in the true value and measured value of a quantity is called error of measurement. (1) Absolute error : Absolute error in the measurement of a physical quantity is the magnitude of the difference between the true value and the measured value of the quantity. Let a physical quantity be measured n times. Let the measured value be \[{{a}_{1}},\,{{a}_{2}},\,{{a}_{3}},\,...\,{{a}_{n}}\]. The arithmetic mean of these value is \[{{a}_{m}}=\frac{{{a}_{1}}+{{a}_{2}}+......+{{a}_{n}}}{n}\] Usually, \[{{a}_{m}}\] is taken as the true value of the quantity, if the same is unknown otherwise. By definition, absolute errors in the measured values of the quantity are \[\Delta {{a}_{1}}={{a}_{m}}-{{a}_{1}}\] \[\Delta {{a}_{2}}={{a}_{m}}-{{a}_{2}}\] ................ \[\Delta {{a}_{n}}={{a}_{m}}-{{a}_{n}}\] The absolute errors may be positive in certain cases and negative in certain other more...

(1) Error in sum of the quantities : Suppose \[x=a+b\] Let \[\Delta a=\] absolute error in measurement of a \[\Delta b=\] absolute error in measurement of b \[\Delta x=\] absolute error in calculation of x i.e. sum of a and b. The maximum absolute error in x is \[\Delta x=\pm (\Delta a+\Delta b)\] Percentage error in the value of \[x=\frac{(\Delta a+\Delta b)}{a+b}\times 100%\] (2) Error in difference of the quantities : Suppose \[x=a-b\] Let \[\Delta a=\] absolute error in measurement of a, \[\Delta b=\] absolute error in measurement of b \[\Delta x=\] absolute error in calculation of x i.e. difference of a and b. The maximum absolute error in x is \[\Delta x=\pm (\Delta a+\Delta b)\] Percentage error in the value of \[x=\frac{(\Delta a+\Delta b)}{a-b}\times 100%\] (3) Error in product of quantities : Suppose \[x=a\times b\] Let \[\Delta a=\] absolute error in measurement of a, \[\Delta b=\] absolute error in measurement more...

When a derived quantity is expressed in terms of fundamental quantities, it is written as a product of different powers of the fundamental quantities. The powers to which fundamental quantities must be raised in order to express the given physical quantity are called its dimensions. To make it more clear, consider the physical quantity force Force = mass × acceleration \[=\frac{\text{mass }\times \text{ velocity}}{\text{time}}\] \[=\frac{\text{mass }\times \text{ length/time}}{\text{time}}\] = mass × length × (time)-2                      ... (i) Thus, the dimensions of force are 1 in mass, 1 in length and - 2 in time. Here the physical quantity that is expressed in terms of the basic quantities is enclosed in square brackets to indicate that the equation is among the dimensions and not among the magnitudes. Thus equation (i) can be written as [force] \[=[ML{{T}^{-2}}]\]. Such an expression for a physical more...

   
Dimension Quantity
\[[{{M}^{0}}{{L}^{0}}{{T}^{-1}}]\] Frequency, angular frequency, angular velocity, velocity gradient and decay constant
\[[{{M}^{1}}{{L}^{2}}{{T}^{-2}}]\] more...
Heat
Quantity Unit Dimension
Temperature (T) Kelvin \[[{{M}^{0}}{{L}^{0}}{{T}^{0}}{{\theta }^{1}}]\]
more...
(1) To find the unit of a physical quantity in a given system of units : To write the definition or formula for the physical quantity we find its dimensions. Now in the dimensional formula replacing M, L and T by the fundamental units of the required system we get the unit of physical quantity. However, sometimes to this unit we further assign a specific name, e.g., Work = Force ´ Displacement So \[[W]=[ML{{T}^{-2}}]\times [L]=[M{{L}^{2}}{{T}^{-2}}]\] So its unit in C.G.S. system will be g \[c{{m}^{2}}/{{s}^{2}}\] which is called erg while in M.K.S. system will be \[kg-{{m}^{2}}/{{s}^{2}}\] which is called joule. (2) To find dimensions of physical constant or coefficients : As dimensions of a physical quantity are unique, we write any formula or equation incorporating the given constant and then by substituting the dimensional formulae of all other quantities, we can find the dimensions of the required constant or coefficient. more...

Although dimensional analysis is very useful it cannot lead us too far as, (1) If dimensions are given, physical quantity may not be unique as many physical quantities have same dimensions. For example if the dimensional formula of a physical quantity is \[[M{{L}^{2}}{{T}^{-2}}]\]it may be work or energy or torque. (2) Numerical constant having no dimensions [K] such as (1/2), 1 or \[2\pi \] etc. cannot be deduced by the methods of dimensions. (3) The method of dimensions can not be used to derive relations other than product of power functions. For example, \[s=u\,t+\,(1/2)\,a\,{{t}^{2}}\] or \[y=a\sin \omega \,t\] cannot be derived by using this theory (try if you can). However, the dimensional correctness of these can be checked. (4) The method of dimensions cannot be applied to derive formula if in mechanics a physical quantity depends on more than 3 physical quantities as then there will be less number (= 3) more...

Significant figures in the measured value of a physical quantity tell the number of digits in which we have confidence. Larger the number of significant figures obtained in a measurement, greater is the accuracy of the measurement. The reverse is also true. The following rules are observed in counting the number of significant figures in a given measured quantity. (1) All non-zero digits are significant. Example :  42.3 has three significant figures.    243.4 has four significant figures.    24.123 has five significant figures. (2) A zero becomes significant figure if it appears between two non-zero digits. Example :  5.03 has three significant figures.                  5.604 has four significant figures.    4.004 has four significant figures. (3) Leading zeros or the zeros placed to the left of the number are never significant. Example : 0.543 has three significant figures.                 0.045 has two significant figures.   0.006 has one more...

While rounding off measurements, we use the following rules by convention: (1) If the digit to be dropped is less than 5, then the preceding digit is left unchanged. Example : \[x=7.82\] is rounded off to 7.8, again \[x=3.94\] is rounded off to 3.9. (2) If the digit to be dropped is more than 5, then the preceding digit is raised by one. Example : x = 6.87 is rounded off to 6.9, again x = 12.78 is rounded off to 12.8. (3) If the digit to be dropped is 5 followed by digits other than zero, then the preceding digit is raised by one. Example : x = 16.351 is rounded off to 16.4, again x = 6.758 is rounded off to 6.8. (4) If digit to be dropped is 5 or 5 followed by zeros, then preceding digit is left unchanged, if it is even. Example : x more...

A quantity which can be measured and by which various physical happenings can be explained and expressed in the form of laws is called a physical quantity. For example length, mass, time, force etc. On the other hand various happenings in life e.g., happiness, sorrow etc. are not physical quantities because these can not be measured. Measurement is necessary to determine magnitude of a physical quantity, to compare two similar physical quantities and to prove physical laws or equations. A physical quantity is represented completely by its magnitude and unit. For example, 10 metre means a length which is ten times the unit of length. Here 10 represents the numerical value of the given quantity and metre represents the unit of quantity under consideration. Thus in expressing a physical quantity we choose a unit and then find that how many times that unit is contained in the given physical quantity, more...


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