We have, $A=\lambda(N)=\frac{0.693}{T_{1 / 2}}(N)$
Initial number of atoms is $A$ and $B$ are same
$\therefore A_{0} \propto \frac{1}{T_{1 / 2}} $
$\Rightarrow \frac{A_{0}(A)}{A_{0}(B)} =\frac{48 hr }{24 hr }=2 $
Also, $A_{0}(A)+A_{0}(B) =1200 $
$\Rightarrow 3 A_{0}(B)=1200 $
$\Rightarrow A_{0}(B)=400$
and $A_{0}(A)=800$
So, $A(A)=\frac{A_{0}(A)}{2^{4}}=\frac{800}{16}=50$
and $A(B)=\frac{A_{0}(B)}{(2)^{2}}=\frac{400}{4}=100$
Hence, total activity after $4$ days is
$=A_{0}(A)+A_{0}(B)=50+100=150$ dis / min
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly:
In the year 1911, Rutherford discovered the atomic nucleus along with his associates. It is already known that every atom is manufactured of positive charge and mass in the form of a nucleus that is concentrated at the center of the atom. More than 99.9% of the mass of an atom is located in the nucleus. Additionally, the size of the atom is of the order of 10-10 m and that of the nucleus is of the order of 10-15 m.
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