R=mN=λ1λ2−λ1R=mN=\frac{λ_1}{λ_2−λ_1}R=mN=λ2−λ1λ1
λ1+λ22=600\frac{λ_1+λ_2}{2}=6002λ1+λ2=600
m=1m=1m=1
N⋅λ2−N⋅λ1=λ1N⋅λ_2−N⋅λ_1=λ_1N⋅λ2−N⋅λ1=λ1
λ1=1200−λ2λ_1=1200−λ_2λ1=1200−λ2
So, we have
1200N−λ1N−λ1N=λ11200N−λ_1N−λ_1N=λ_11200N−λ1N−λ1N=λ1
1200N=λ1(2N+1)1200N=λ_1(2N+1)1200N=λ1(2N+1)
λ1=1200N2N+1=1200⋅20002⋅2000+1=599.85nmλ1=\frac{1200N}{2N+1}=\frac{1200\cdot 2000}{2\cdot 2000+1}=599.85nmλ1=2N+11200N=2⋅2000+11200⋅2000=599.85nm
λ2=1200−599.85=600.15nmλ_2=1200−599.85=600.15nmλ2=1200−599.85=600.15nm
λ2−λ1=600.15−599.85=0.3nmλ_2−λ_1=600.15−599.85=0.3nmλ2−λ1=600.15−599.85=0.3nm
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