If the measurement errors in all the independent quantities are known, then it is possible to determine the error in any dependent quantity. This is done by the use of series expansion and truncating the expansion at the first power of the error. For example, consider the relation `z=x//y`.If the errors in x, y and z are `Delta x, Delta y and Delta z`, respectively, then
`zpm Deltaz =(x pm Delta x)/(y pm Delta y)=(x)/(y)(1pm(Deltax)/(x))(1pm(Delta y)/(y))^(-1)`.
The series expansion for `(1pm (Delta y)/(y))^(-1)`, to first power in `Delta y//y. " is " 1 pm (Delta y//y)`. The relative errors in independent variables are always added. So the error in z will be
`Delta z =z((Delta x)/(x)+(Delta y)/(y))`.
The above derivation makes the assumption that `Delta x// x lt lt 1, Delta y //y lt lt 1`. Therefore, the higher powers of these quantities are neglected.
In an experiment the initial number of radioactive nuclei is 3000. It is found that `1000 pm 40` nuclei decayed in the first 1.0 s. For `| x| lt lt 1, "In"(1+x)=x` up to first power in x. The error `Delta lambda`, in the determination of the decay constant `lambda, " in " s^(-1)`, is

Options

A. 0.04
B. 0.03
C. 0.02
D. 0.01

Answer

C

Explanation

`N=N_(0)e^(-lambdat)`
`lnN=lnN_(0)-lambdat`
Differentiate w.r.t `lambda`
`1/N(dN)/(dlambda)=0-t`
`dlambda =(dN)/(dt) =40/(2000 xx 1) = 0.02`