Physics, asked by Anonymous, 7 months ago

Question :

When a charged particle of charge x C moves through a potential Difference of y V , the gain in Kinetic energy is equal to xy J.

An electron and an alpha particle have their masses in the ratio of 1 : 7200 and charges in the ratio of 1 : 2 . If they start moving from rest through the same electrical Potential Difference , find the ratio of their Velocities.

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Answers

Answered by Anonymous
17

Given :

If particle has charge x coulombs and potential difference y volts . Then gain in K.E. = xy joules.

Using similar analysis,

 \frac{(mass)electron}{(mass)alpha \:  \: electron}  =  \frac{1}{7200}  \\  \\  \frac{charge \:  \: electron}{charge \:  \: alpha \:  \: electron}  =  \frac{1}{2}

Since initially there at rest, initial K.E. = 0;

They move through same potential difference. Let potential difference be y volts.

So, gain in K.E = Final K.E – Initial K.E

= Final K.E – 0

So, gain in K.E = charge×potentialdifference

Ratio of gain in K.E of electron and α particle = Ratio of final K.E of electron and α particles .

 =  \frac{ \frac{1}{2} {mv}^{2}_e \times y  }{ \frac{1}{2}  {mv}^{2} _ \alpha  \times y}  \\  \\  =  \frac{1}{2}  \times 7200 = 3600 \\  \\

 \frac{V_e}{V_ \alpha } =  \sqrt{3600}   = 60 \\  \\

°Ratio is 60:1

Answered by Ekaro
25

Given :

For an electron and an alpha particle;

Ratio of masses = 1:7200

Ratio of charges = 1:2

Both start moving from rest through the same electrical potential.

To Find :

We have to find ratio of their velocities.

Solution :

Mechanical kinetic energy

  • K(m) = 1/2 mv²

Electrical kinetic energy

  • K(e) = eV

where,

m denotes mass of particle

v denotes velocity of particle

e denotes charge of particle

V denotes potential difference

\sf{\dfrac{\frac{1}{2}\times m_1v_1^2}{\frac{1}{2}\times m_2v_2^2} = \dfrac{e_1V_1}{e_2V_2}}

ATQ,

  • m₁ : m₂ =1 : 7200
  • e₁ : e₂ = 1 : 2
  • V₁ = V₂ = V

➠ m₁/m₂ × v₁²/v₂² = e₁/e₂

➠ 1/7200 × v₁²/v₂² = 1/2

➠ v₁²/v₂² = 7200/2

➠ v₁/v₂ = √3600

v₁ : v₂ = 60 : 1

Cheers!


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