Question #105753

Millikan's oil drop experiment the mass of the oil drops is obtained by observing the terminals Vt of a freely falling drop in the absence of an electric field. under the circumstances the effective weight equals the viscous Force given by stroke's law F= 6ie ΠrVr where Π is 1.8 * 10 - 5 kg/m.s is the viscosity of air and r is 0.65 cm is the of the radius of the drop . Also the actual with Mg =⁴÷² pie r³ density gram. must be corrected for the buoyant force of the air this is done by replacing density with density -densityA .density is 9.20 x 10² kg/m³ the density of the oil and density is 1.29 kg/m³ density of air with this premier a show that charge drop is given by

Expert's answer

As per the given question,


F=6πηrVtF=6\pi \eta rV_t

η=1.8×10−5kg/m.s\eta= 1.8\times 10^{ - 5} kg/m.s

radius (r)=0.65cm

Density of oil drop ρoil=9.20×102kg/m3\rho_{oil}=9.20 \times 10^2 kg/m^3

Density of the airρair=1.29×102kg/m3\rho_{air}=1.29 \times 10^{2}kg/m^3

We know that,

downward force =Upward force

Let the mass of the drop is M and g is the gravitational acceleration, FthF_{th} is the thrust force on the drop, let V is the volume of the drop is V,

So, Mg−Fth=6πηrVtMg-F_{th}=6\pi \eta rV_t

⇒Vt=Mg−ρair×V6πηr\Rightarrow V_t=\dfrac{Mg-\rho_{air}\times V}{6\pi \eta r}

⇒Vt=V(ρoil−ρair)6πηr\Rightarrow V_t=\dfrac{V(\rho_{oil}-\rho_{air})}{6\pi \eta r}

Now, substituting the values in the above,

Vt=(ρoil−ρair)×43×πr36πηrV_t=\dfrac{(\rho_{oil}-\rho_{air}) \times \dfrac{4}{3}\times \pi r^3}{6\pi \eta r}


⇒Vt=2(ρoil−ρair)πr29π×η=(ρoil−ρair)r29η\Rightarrow V_t=\dfrac{2(\rho_{oil}-\rho_{air}) \pi r^2}{9\pi\times \eta}=\dfrac{(\rho_{oil}-\rho_{air}) r^2}{9\eta}


⇒Vt=2×(9.20−1.29)×102×0.65×10−26×1.8×10−5\Rightarrow V_t=\dfrac{2\times(9.20-1.29)\times 10^{2}\times 0.65\times 10^{-2}}{6\times 1.8\times 10^{-5}} m/sec


Vt=2×7.91×0.659×10−5=10.283×1059m/secV_t=\dfrac{2\times 7.91\times 0.65}{9\times 10^{-5}}=\dfrac{10.283\times 10^{5}}{9}m/sec

⇒Vt=1.14×105m/sec\Rightarrow V_t=1.14\times10^{5} m/sec



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