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At the suggestion of Earnest Rutherford,...

At the suggestion of Earnest Rutherford, hans Geiger and ernest Marsden bombarded a thin gold foil by `alpha`-particles from a polonium source. It was expected that `alpha`-particles would go right through the foil with hardly any deflection. Although, most of the alpha particles indeed were not deviated by much, a few were scattered through veryi large angles. Some were even scattered in the backward direction. The nly way to explain the results, rutherford found, was to picture an atom as being compoed of a tiny nucleus in which its positive charge and nearly all its mass are concentrated. Scattering of `alpha`-particles is proportional to target thickness and is inversely proportional to the fourth power of `sin((theta)/(2))`, where,` theta` is scattering angle. Distance of closest approach may be calculated as:
`r_("min")=(Z_(1)Z_(2)e^(2))/(4piepsi_(0)K)`
where, K=kinetic energy of `alpha`-particles.
Q. Rutherford's `alpha`-particle scattering led to the conclusion that:

A

mass and energy are related

B

mass and postive charge of an atom are concentrated in the nucleus

C

neutrons are present I the nucleus

D

atoms are electrically neutrally

Text Solution

Verified by Experts

The correct Answer is:
B
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At the suggestion of Ernest Rutherford, Hans Geiger and Ernest Marsden bombarded a thin gold foil by d-particles from a polonium source. It was expected that O-particles would go right through the foil with hardly any deflection. Although most of the alpha particles indeed were not deviated by much, a few were scattered through very large angles. Some were even scattered in the backward direction. The only way to explain the results Rutherford found, was to picture an atom as being composed of a tiny nucleus in which it is positive charge and nearly all its mass is concentrated. Alpha particles that come closer to the nuclei

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Knowledge Check

  • At the suggestion of Earnest Rutherford, hans Geiger and ernest Marsden bombarded a thin gold foil by alpha -particles from a polonium source. It was expected that alpha -particles would go right through the foil with hardly any deflection. Although, most of the alpha particles indeed were not deviated by much, a few were scattered through veryi large angles. Some were even scattered in the backward direction. The nly way to explain the results, rutherford found, was to picture an atom as being compoed of a tiny nucleus in which its positive charge and nearly all its mass are concentrated. Scattering of alpha -particles is proportional to target thickness and is inversely proportional to the fourth power of sin((theta)/(2)) , where, theta is scattering angle. Distance of closest approach may be calculated as: r_("min")=(Z_(1)Z_(2)e^(2))/(4piepsi_(0)K) where, K=kinetic energy of alpha -particles. Q. Alpha particles that come closer to the nuclei:

    A
    are deflected more
    B
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    C
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    D
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  • At the suggestion of Earnest Rutherford, hans Geiger and ernest Marsden bombarded a thin gold foil by alpha -particles from a polonium source. It was expected that alpha -particles would go right through the foil with hardly any deflection. Although, most of the alpha particles indeed were not deviated by much, a few were scattered through veryi large angles. Some were even scattered in the backward direction. The nly way to explain the results, rutherford found, was to picture an atom as being compoed of a tiny nucleus in which its positive charge and nearly all its mass are concentrated. Scattering of alpha -particles is proportional to target thickness and is inversely proportional to the fourth power of sin((theta)/(2)) , where, theta is scattering angle. Distance of closest approach may be calculated as: r_("min")=(Z_(1)Z_(2)e^(2))/(4piepsi_(0)K) where, K=kinetic energy of alpha -particles. Q. Which of the following quantities will be zero for alpha particles at the point of closest approach to the gold atom, in Rutherford's scattering of alpha particles?

    A
    Acceleration
    B
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    C
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    D
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  • At the suggestion of Earnest Rutherford, hans Geiger and ernest Marsden bombarded a thin gold foil by alpha -particles from a polonium source. It was expected that alpha -particles would go right through the foil with hardly any deflection. Although, most of the alpha particles indeed were not deviated by much, a few were scattered through veryi large angles. Some were even scattered in the backward direction. The nly way to explain the results, rutherford found, was to picture an atom as being compoed of a tiny nucleus in which its positive charge and nearly all its mass are concentrated. Scattering of alpha -particles is proportional to target thickness and is inversely proportional to the fourth power of sin((theta)/(2)) , where, theta is scattering angle. Distance of closest approach may be calculated as: r_("min")=(Z_(1)Z_(2)e^(2))/(4piepsi_(0)K) where, K=kinetic energy of alpha -particles. Q. Rutherford's scattering formula fails for vary small scattering angles because:

    A
    The gold foil is very thin
    B
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    C
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    D
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    At the suggestion of Ernest Rutherford, Hans Geiger and Ernest Marsden bombarded a thin gold foil by d-particles from a polonium source. It was expected that O-particles would go right through the foil with hardly any deflection. Although most of the alpha particles indeed were not deviated by much, a few were scattered through very large angles. Some were even scattered in the backward direction. The only way to explain the results Rutherford found, was to picture an atom as being composed of a tiny nucleus in which it is positive charge and nearly all its mass is concentrated. The C-particle scattering experiment led to the conclusion that

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