Physics

$A=\frac{A_0}{16}=\frac{A_0}{2^{30/t_{1/2}}}\Rightarrow 2^4=2^{30/t_{1/2}}$

$\Rightarrow \frac{A_0}{16}=\frac{A_0}{2^{30/t_{1/2}}}\Rightarrow 2^4=2^{30/t_{1/2}}$

$\Rightarrow t_{1/2}=\frac{30}{4}=7.5$ years

Given that   $\overrightarrow{v}=v_{0}iand\overrightarrow{E}=-E_0\widehat{i}$

  $\overrightarrow{v}\left(t\right)=v_0\widehat{i}+\frac{eEt}{m}\widehat{i}$              

So, de Broglie wave length,   $\lambda =\frac{h}{mv}$

$\Rightarrow \lambda =\frac{h}{m{v}_0\left(1+\frac{q{E}_0}{m{v}_0}t\right)}=\frac{{\lambda }_0}{\left(1+\frac{q{E}_0}{m{v}_0}t\right)}$

Resolving power

$E_y=900sin\omega \left(t-\raisebox{1ex}{$x$}\!\left/ \!\raisebox{-1ex}{$c$}\right.\right)$

$\frac{F_E}{F_B}=\frac{qE}{\left|q\overline{V}*\overline{B}\right|}=\frac{C}{V}=\frac{3*10^8}{3*10^7}=10$

$\Rightarrow \frac{F_E}{F_B}=\frac{10}{1}$

In DC :-                In AC:-

              i₁ = 4A                 i₂ = 4 sin   $\omega t$

              R₁ = 3   $\Omega$             R₂ =   $2\Omega$

              In same time internal of 't' - $\frac{H_1}{H_2}=\frac{i_1^2{R}_{1}t}{{\left({\mathcal{l}}_{2^{-rms}}\right)}^2{R}_{2}t}=\frac{16*3t}{{\left(\frac{4}{\sqrt[]{2}}\right)}^2*2*t}=\frac{48}{\left(\frac{32}{2}\right)}=3:1$

Let angle of dip =

Then B cos 45° = B' cos 60°- (i)

B' sin 60 = B sin - (ii)

$\left(i\right)÷\left(ii\right)\Rightarrow cost60=cot\alpha cos45°$

$cot\alpha =\frac{cot60°}{cos45°}=\frac{1\sqrt[]{2}}{\sqrt[]{3}x}=\sqrt[]{\frac{2}{3}}$

$tan\alpha =\sqrt[]{\frac{3}{2}}$

$\alpha =ta{n}^{-1}\sqrt[]{\frac{3}{2}}$

T₁ = 3 sec T₂ = 4sec

$T=2\pi \sqrt[]{\frac{I}{\mu B}}$

$\frac{I_1}{I_2}=\frac{3}{2}\Rightarrow \frac{T_1}{T_2}=\sqrt[]{\frac{l_1{\mu }_2}{{\mu }_1{l}_2}}$

$\Rightarrow {\left(\frac{3}{4}\right)}^2=\frac{I_1}{I_2}\left(\frac{{\mu }_2}{{\mu }_1}\right)\Rightarrow \frac{{\mu }_2}{{\mu }_1}=\frac{l_2}{l_1}*\frac{9}{16}=\frac{2}{3}*\frac{9}{16}=\frac{3}{8}$ $\Rightarrow \frac{{\mu }_1}{{\mu }_2}=\frac{8}{3}$

V_AB = 0

$or,\epsilon -i{r}_1=0$

$\Rightarrow \epsilon -\frac{2\epsilon }{r_1+r_2+R}{r}_1=0\Rightarrow 1=\frac{2r_1}{r_1+r_2+R}$

$\Rightarrow R+r_1+r_2=2r_1$

$R=r_1-r_2$

$F_R=\left\{\frac{kQ{q}_0}{{\left(a-x\right)}^2}-\frac{kQ{q}_0}{{\left(a+x\right)}^2}\right\}$

$=-kQ{q}_0\left\{\frac{a^2+x^2+2ax-a^2-x^2+2ax}{\left(a^2-x^2\right)}\right\}$

$F_R=-\frac{kQ{q}_0\left(4ax\right)}{{\left(a^2-x^2\right)}^2}$

$T=2\pi \sqrt[]{\frac{a^{3}m}{4kQ{q}_0}=\sqrt[]{\frac{4{\pi }^2{a}^{3}m*4\pi {\epsilon }_0}{4Q{q}_0}}}=\sqrt[]{\frac{4{\pi }^3{\epsilon }_{0}m{a}^3}{Q{q}_0}}$

$V_{rms}=\sqrt[]{\frac{3RT}{M}}As.v_1=v_2$

$V_{rms}\alpha \sqrt[]{T}$       ${\eta }_2=4n_1$

$T_1=T_2\Rightarrow V_{rms-1}=V_{rms-2}$

$P_1=\frac{n_{1}RT}{v}{P}_z=\frac{n_{2}RT}{v}$

$\frac{P_1}{P_2}=\frac{n_1}{n_2}=\frac{1}{4}$