NEET Physics Atoms MCQs

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    NEET Questions / Physics / Atoms

    3.

    A diatomic molecule is made of two masses m1{m_1} and m2{m_2} which are separated by a distance rr. If we calculate its rotational energy by applying Bohr’s rule of angular momentum quantization, its energy will be given by (nn is an integer)

    A

    (m1+m2)2n2h22 m12 m22r2\frac{{{{\left( {{m_1} + {m_2}} \right)}^2}{n^2}{h^2}}}{{2\,m_1^2\,m_2^2{r^2}}}

    B

    n2h22(m1+m2)r2\frac{{{n^2}{h^2}}}{{2\left( {{m_1} + {m_2}} \right){r^2}}}

    C

    2 n2h2(m1+m2)r2\frac{{2\,{n^2}{h^2}}}{{\left( {{m_1} + {m_2}} \right){r^2}}}

    D

    (m1+m2)n2h22 m1 m2r2\frac{{{{\left( {{m_1} + {m_2}} \right)}^{}}{n^2}{h^2}}}{{2\,{m_1}\,{m_2}{r^2}}}

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    4.

    A diatomic molecule is made of two masses m1{m_1} and m2{m_2} which are separated by a distance rr. If we calculate its rotational energy by applying Bohr’s rule of angular momentum quantization, its energy will be given by (nn is an integer)

    A

    (m1+m2)2n2h22 m12 m22r2\frac{{{{\left( {{m_1} + {m_2}} \right)}^2}{n^2}{h^2}}}{{2\,m_1^2\,m_2^2{r^2}}}

    B

    n2h22(m1+m2)r2\frac{{{n^2}{h^2}}}{{2\left( {{m_1} + {m_2}} \right){r^2}}}

    C

    2 n2h2(m1+m2)r2\frac{{2\,{n^2}{h^2}}}{{\left( {{m_1} + {m_2}} \right){r^2}}}

    D

    (m1+m2)n2h22 m1 m2r2\frac{{{{\left( {{m_1} + {m_2}} \right)}^{}}{n^2}{h^2}}}{{2\,{m_1}\,{m_2}{r^2}}}

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    6.

    A diatomic molecule is made of two masses m1{m_1} and m2{m_2} which are separated by a distance rr. If we calculate its rotational energy by applying Bohr’s rule of angular momentum quantization, its energy will be given by (nn is an integer)

    A

    (m1+m2)2n2h22 m12 m22r2\frac{{{{\left( {{m_1} + {m_2}} \right)}^2}{n^2}{h^2}}}{{2\,m_1^2\,m_2^2{r^2}}}

    B

    n2h22(m1+m2)r2\frac{{{n^2}{h^2}}}{{2\left( {{m_1} + {m_2}} \right){r^2}}}

    C

    2 n2h2(m1+m2)r2\frac{{2\,{n^2}{h^2}}}{{\left( {{m_1} + {m_2}} \right){r^2}}}

    D

    (m1+m2)n2h22 m1 m2r2\frac{{{{\left( {{m_1} + {m_2}} \right)}^{}}{n^2}{h^2}}}{{2\,{m_1}\,{m_2}{r^2}}}

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    7.

    In a hypothetical Bohr hydrogen, the mass of the electron is doubled. The energy E0{E_0} and the radius r0{r_0} of the first orbit will be (a0{a_0} is the Bohr radius)

    A

    E0=βˆ’27.2  eV;  r0=a0/2{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}/2

    B

    E0=βˆ’27.2  eV;  r0=a0{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}

    C

    E0=βˆ’13.6  eV;  r0=a0/2{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}/2

    D

    E0=βˆ’13.6  eV;  r0=a0{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}

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    8.

    In a hypothetical Bohr hydrogen, the mass of the electron is doubled. The energy E0{E_0} and the radius r0{r_0} of the first orbit will be (a0{a_0} is the Bohr radius)

    A

    E0=βˆ’27.2  eV;  r0=a0/2{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}/2

    B

    E0=βˆ’27.2  eV;  r0=a0{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}

    C

    E0=βˆ’13.6  eV;  r0=a0/2{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}/2

    D

    E0=βˆ’13.6  eV;  r0=a0{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}

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    9.

    In a hypothetical Bohr hydrogen, the mass of the electron is doubled. The energy E0{E_0} and the radius r0{r_0} of the first orbit will be (a0{a_0} is the Bohr radius)

    A

    E0=βˆ’27.2  eV;  r0=a0/2{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}/2

    B

    E0=βˆ’27.2  eV;  r0=a0{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}

    C

    E0=βˆ’13.6  eV;  r0=a0/2{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}/2

    D

    E0=βˆ’13.6  eV;  r0=a0{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}

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    10.

    In a hypothetical Bohr hydrogen, the mass of the electron is doubled. The energy E0{E_0} and the radius r0{r_0} of the first orbit will be (a0{a_0} is the Bohr radius)

    A

    E0=βˆ’27.2  eV;  r0=a0/2{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}/2

    B

    E0=βˆ’27.2  eV;  r0=a0{E_0} = - 27.2\,\,eV;\,\,{r_0} = {a_0}

    C

    E0=βˆ’13.6  eV;  r0=a0/2{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}/2

    D

    E0=βˆ’13.6  eV;  r0=a0{E_0} = - 13.6\,\,eV;\,\,{r_0} = {a_0}

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