Home
Class 11
PHYSICS
A physical quantity X depends on another...

A physical quantity X depends on another physical quantities as `X=YFe^(-beta r^(2))+ZW sin (alpha r)` where r, F and W represents distance, force and work respectively & Y and Z are unknown physical quantities and `alpha, beta` are positive contsnats.
If Y respresent displacement then `dim((alphaYZ)/(betaF))` is equal to

A

`M^(-1) LT^(2)`

B

`M^(-1) L^(2)T^(-2)`

C

`M^(1) L^(1) T^(-2)`

D

None of these

Text Solution

Verified by Experts

The correct Answer is:
A

Given `" "X=Yfe^(-betar^(2))+ZW sin (alphar) " "` Here `Dim (beta)=L^(-2), Dim (alpha)=L^(-1)`
Also `" " Dim (X)=Dim(YE)` …(i) & `" "Dim (X)=Dim(ZW)` …(ii)
Now If `" " Dim (Y)=L`
So `" " Dim(X)=[LMLT^(-2)]=[ML^(2)T^(-2)]" "` from equation (i)
and `" " Dim(Z)=Dim(X/W)=[(ML^(2)T^(-2))/(ML^(2)T^(-2))]=[M^(0)L^(0)T^(0)]" "` from equation (ii)
Thus`" "Dim((alphaYZ)/(betaF))=[(L^(-1)L)/(L^(-2)MLT^(-2))]=[M^(-1)LT^(2)]`
Promotional Banner

Topper's Solved these Questions

  • MISCELLANEOUS

    ALLEN |Exercise Part -II Example|61 Videos
  • MISCELLANEOUS

    ALLEN |Exercise Part -II Example Some worked out Examples|1 Videos
  • KINEMATICS (MOTION ALONG A STRAIGHT LINE AND MOTION IN A PLANE)

    ALLEN |Exercise BEGINNER S BOX-7|8 Videos
  • PHYSICAL WORLD, UNITS AND DIMENSIONS & ERRORS IN MEASUREMENT

    ALLEN |Exercise EXERCISE-IV|7 Videos

Similar Questions

Explore conceptually related problems

A physical quantity X depends on another physical quantities as X=YFe^(-beta r^(2))+ZW sin (alpha r) where r, F and W represents distance, force and work respectively & Y and Z are unknown physical quantities and alpha, beta are positive contsnats. If T represent velocity then dim (X) is equal to

A physical quantity X depends on another physical quantities as X=YFe^(-beta r^(2))+ZW sin (alpha r) where r, F and W represents distance, force and work respectively & Y and Z are unknown physical quantities and alpha, beta are positive contsnats. If Z represent frequency then choose the correct alternative

A physical quantity is given by X=[M^(a)L^(b)T^(c)] . The percentage error in measurement of M,L and T are alpha, beta, gamma respectively. Then the maximum % error in the quantity X is

The unit of three physical quantities x, y and z are g cm^(2) s^(-5) , gs^(-1) and cm s^(-2) respectively. The relation between x, y and z is

A physical quantity X is represented by X = (M^(x) L^(-y) T^(-z) . The maximum percantage errors in the measurement of M , L , and T , respectively , are a% , b% and c% . The maximum percentage error in the measurement of X will be

Vector vecP angle alpha,beta and gamma with the x,y and z axes respectively. Then sin^(2)alpha+sin^(2)beta+sin^(2)gamma=

If a vector vec(A) make angles alpha , beta and gamma , respectively , with the X , Y and Z axes , then sin^(2) alpha + sin^(2) beta + sin^(2) gamma =

Let y = f(x), f : R ->R be an odd differentiable function such that f'''(x)>0 and g(alpha,beta)=sin^8alpha+cos^8beta+2-4sin^2alpha cos^2 beta If f''(g(alpha, beta))=0 then sin^2alpha+sin^2beta is equal to

Let alpha, beta in R such that lim_(x ->0) (x^2sin(betax))/(alphax-sinx)=1 . Then 6(alpha + beta) equals

A physical quantity is a phyical property of a phenomenon , body, or substance , that can be quantified by measurement. The magnitude of the components of a vector are to be considered dimensionally distinct. For example , rather than an undifferentiated length unit L, we may represent length in the x direction as L_(x) , and so forth. This requirement status ultimately from the requirement that each component of a physically meaningful equation (scaler or vector) must be dimensionally consistent . As as example , suppose we wish to calculate the drift S of a swimmer crossing a river flowing with velocity V_(x) and of widht D and he is swimming in direction perpendicular to the river flow with velocity V_(y) relation to river, assuming no use of directed lengths, the quantities of interest are then V_(x),V_(y) both dimensioned as (L)/(T) , S the drift and D width of river both having dimension L. with these four quantities, we may conclude tha the equation for the drift S may be written : S prop V_(x)^(a)V_(y)^(b)D^(c) Or dimensionally L=((L)/(T))^(a+b)xx(L)^(c) from which we may deduce that a+b+c=1 and a+b=0, which leaves one of these exponents undetermined. If, however, we use directed length dimensions, then V_(x) will be dimensioned as (L_(x))/(T), V_(y) as (L_(y))/(T), S as L_(x)" and " D as L_(y) . The dimensional equation becomes : L_(x)=((L_(x))/(T))^(a) ((L_(y))/(T))^(b)(L_(y))^(c) and we may solve completely as a=1,b=-1 and c=1. The increase in deductive power gained by the use of directed length dimensions is apparent. From the concept of directed dimension what is the formula for a range (R) of a cannon ball when it is fired with vertical velocity component V_(y) and a horizontal velocity component V_(x) , assuming it is fired on a flat surface. [Range also depends upon acceleration due to gravity , g and k is numerical constant]