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Question: Conductivity of a saturated solution of \[C{u_2}\left[ {Fe{{\left( {CN} \right)}_6}} \right]\] after...

Conductivity of a saturated solution of Cu2[Fe(CN)6]C{u_2}\left[ {Fe{{\left( {CN} \right)}_6}} \right] after subtracting the conductivity of water is 1.28×105Ω1cm11.28 \times {10^{ - 5}}{\Omega ^{ - 1}}c{m^{ - 1}}.Calculate value of solubility of Cu2[Fe(CN)6]C{u_2}\left[ {Fe{{\left( {CN} \right)}_6}} \right]
Λmx(CuSO4)=260Scm2mol1\Lambda mx\left( {CuS{O_4}} \right) = 260Scm2mo{l^{ - 1}}
Λmx(K2SO4)=300Scm2mol1\Lambda mx\left( {{K_2}S{O_4}} \right) = 300Scm2mo{l^{ - 1}}
Λmx(K4Fe(CN)6)=720Scm2mol1\Lambda mx\left( {{K_4}Fe{{\left( {CN} \right)}_6}} \right) = 720Scm2mo{l^{ - 1}}
Report your answer as (solubility) ×(105) \times \left( {{{10}^5}} \right)

Explanation

Solution

We know that Conductivity is the proportion of the simplicity at which an electric charge or warmth can go through a material. A transmitter is a material which gives next to no protection from the progression of an electric flow or nuclear power. Materials are delegated metals, semiconductors, and encasings.

Complete answer:
We must know that electrical resistivity (additionally called explicit electrical opposition or volume resistivity) is a central property of a material that acts unequivocally against electric flow. Its converse, called electrical conductivity, evaluates how well a material behaves. A low resistivity demonstrates a material that promptly permits electric flow. Resistivity is generally addressed by the Greek letter ρ (rho). The SI unit of electrical resistivity is the ohm-meter. For instance, if a one meter strong 3D shape of material has sheet contacts on two inverse countenances, and the opposition between these contacts is one ohm, at that point the resistivity of the material is 11 ohm meter.
The balanced chemical equation for the given reaction is,
K4Fe(CN)6+2CuSO4Cu2[Fe(CN6)]+2H2SO4{K_4}Fe{\left( {CN} \right)_6} + 2CuS{O_4} \to C{u_2}\left[ {Fe\left( {C{N_6}} \right)} \right] + 2{H_2}S{O_4}
The conductivity of the given complex is calculated as,
λmCu2[Fe(CN)6]=λmK4Fe(CN)6+2λmCuSO42λmK2SO4{\lambda _m}C{u_2}\left[ {Fe{{\left( {CN} \right)}_6}} \right] = {\lambda _m}{K_4}Fe{\left( {CN} \right)_6} + 2{\lambda _m}CuS{O_4} - 2{\lambda _m}{K_2}S{O_4}
Now we can substitute the known values we get,
λm=720+2(260)2(300){\lambda _m} = 720 + 2\left( {260} \right) - 2\left( {300} \right)
On simplification we get,
λm=640scm2mol1{\lambda _m} = 640sc{m^2}mo{l^{ - 1}}

Additional information:
We know that the electrical conductivity or explicit conductance is the complementary of electrical resistivity. It addresses a material's capacity to channel electric flow. It is usually implied by the Greek letter σ\sigma (sigma), yet KK (kappa) (particularly in electrical designing) and γ\gamma (gamma) are at times utilized. The SI unit of electrical conductivity is Siemens per meter (S/m).

Note:
Conductivity may allude to:
Electrical conductivity, a proportion of a material's capacity to direct an electric flow
Conductivity (electrolytic), the electrical conductivity of an electrolyte in arrangement
Ionic conductivity (strong state), electrical conductivity because of particles moving situation in a precious stone cross section
Pressure driven conductivity, a property of a permeable material's capacity to send water
Thermal conductivity, a serious property of a material that shows its capacity to lead heat.