Atomic Structure and Hydrogen Atom
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Atomic Structure and Hydrogen Atom

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The size of the atom in Thomson's model is ______ the atomic size in Rutherford's model.

  • much greater than (correct)
  • no different from
  • much less than
  • In the ground state of ______ electrons are in stable equilibrium, while in ______ electrons always experience a net force.

  • Rutherford's model/ Thomson's model
  • Thomson's model/ Rutherford's model (correct)
  • A classical atom based on ______ is doomed to collapse.

  • Rutherford's model (correct)
  • Thomson's model
  • An atom has a nearly continuous mass distribution in ______ but has a highly non-uniform mass distribution in ______.

    <p>Thomson's model/ Rutherford's model</p> Signup and view all the answers

    The positively charged part of the atom possesses most of the mass in ______.

    <p>Rutherford's model</p> Signup and view all the answers

    Suppose you are given a chance to repeat the alpha-particle scattering experiment using a thin sheet of solid hydrogen in place of the gold foil. (Hydrogen is a solid at temperatures below 14 K.) What results do you expect?

    <p>Since hydrogen has a much lighter nucleus compared to gold, the alpha particles would be deflected by much smaller angles, meaning that most of the alpha particles would pass through the hydrogen foil without significant deflection. The number of particles scattered backwards would be very low.</p> Signup and view all the answers

    A difference of 2.3 eV separates two energy levels in an atom. What is the frequency of radiation emitted when the atom makes a transition from the upper level to the lower level?

    <p>The frequency of the emitted radiation can be calculated using the relationship: hv = E_i - E_f, where h is Planck's constant (6.63 × 10^-34 Js), v is the frequency, and E_i and E_f are the energies of the initial and final states, respectively. Converting the energy difference of 2.3 eV to joules (1 eV = 1.602 × 10^-19 J) and plugging the values into the equation, we get: v = (2.3 × 1.602 × 10^-19 J) / (6.63 × 10^-34 Js) = 5.56 × 10^14 Hz.</p> Signup and view all the answers

    The ground state energy of the hydrogen atom is -13.6 eV. What are the kinetic and potential energies of the electron in this state?

    <p>The total energy of the electron in the ground state is -13.6 eV. This energy is the sum of its kinetic energy (K) and potential energy (U). The kinetic energy of the electron is half its potential energy, so K = -13.6 eV / 2 = -6.8 eV. The potential energy is then U = -13.6 eV - (-6.8 eV) = -6.8 eV.</p> Signup and view all the answers

    A hydrogen atom initially in the ground level absorbs a photon, which excites it to the n = 4 level. Determine the wavelength and frequency of the photon.

    <p>The energy difference between the n=4 and n=1 levels in a hydrogen atom is 12.75 eV. Therefore, the photon absorbed by the atom has an energy of 12.75 eV. Using the relationship E = hc/λ, where h is Planck's constant (6.63 × 10^-34 Js), c is the speed of light (3 × 10^8 m/s), and λ is the wavelength, we can calculate the wavelength of the photon: λ = hc/E = (6.63 × 10^-34 Js)(3 × 10^8 m/s) / (12.75 × 1.602 × 10^-19 J) = 9.72 × 10^-8 m = 97.2 nm. The frequency of the photon can be calculated using the equation ν = c/λ = (3 × 10^8 m/s) / (9.72 × 10^-8 m) = 3.09 × 10^15 Hz.</p> Signup and view all the answers

    Using the Bohr's model, calculate the speed of the electron in a hydrogen atom in the n = 1, 2, and 3 levels. Calculate the orbital period in each of these levels.

    <p>The speed of the electron in the nth Bohr orbit is given by v = (e^2)/(2ε_0hn) = (1.602 × 10^-19 C)^2 / (2 × 8.85 × 10^-12 C^2/(Nm^2) × 6.63 × 10^-34 Js × n). Substituting the values for n = 1, 2, and 3, we get: v_1 = 2.19 × 10^6 m/s, v_2 = 1.09 × 10^6 m/s, and v_3 = 7.3 × 10^5 m/s. The orbital period (T) in the nth Bohr orbit is given by T = (2πr_n)/v, where r_n is the radius of the nth Bohr orbit. Substituting the value of r_n = n^2 a_0, where a_0 is the Bohr radius (5.29 × 10^-11 m), we get: T_1 = (2π) × (5.29 × 10^-11 m) / (2.19 × 10^6 m/s) = 1.52 × 10^-16 s, T_2 = (2π) × (4 × 5.29 × 10^-11 m) / (1.09 × 10^6 m/s) = 1.22 × 10^-15 s, and T_3 = (2π) × (9 × 5.29 × 10^-11 m) / (7.3 × 10^5 m/s) = 3.88 × 10^-15 s.</p> Signup and view all the answers

    The radius of the innermost electron orbit of a hydrogen atom is 5.3 × 10^-11 m. What are the radii of the n = 2 and n = 3 orbits?

    <p>The radii of the orbits in the Bohr model are quantized and directly proportional to the square of the principal quantum number (n). Therefore, the radius of the n = 2 orbit is 2^2 * 5.3 × 10^-11 m = 2.12 × 10^-10 m, and the radius of the n = 3 orbit is 3^2 * 5.3 × 10^-11 m = 4.8 × 10^-10 m.</p> Signup and view all the answers

    A 12.5 eV electron beam is used to bombard gaseous hydrogen at room temperature. What series of wavelengths will be emitted?

    <p>When a hydrogen atom absorbs energy from an electron beam, its electron can be excited to higher energy states. The electron will eventually transition back to lower energy states, emitting photons with energies equal to the energy differences between these states. The 12.5 eV electron beam has enough energy to excite the electron to the n = 2 or higher levels. Therefore, the emitted photons will correspond to transitions from these higher levels to the n = 1 level, resulting in the emission of the Lyman series, which is characterized by ultraviolet wavelengths.</p> Signup and view all the answers

    In accordance with the Bohr's model, find the quantum number that characterizes the earth's revolution around the sun in an orbit of radius 1.5 × 10^11 m with orbital speed 3 × 10^4 m/s. (Mass of earth = 6.0 × 10^24 kg).

    <p>To find the quantum number (n) that characterizes Earth's orbit around the Sun using Bohr's model, we can apply the quantization condition for angular momentum: mvr = nh/2π. Given the radius (r) of the orbit is 1.5 × 10^11 m, the speed (v) of Earth is 3 × 10^4 m/s, and the mass (m) of Earth is 6.0 × 10^24 kg, Planck's constant (h) is 6.63 × 10^-34 Js. Plugging these values into the equation yields: n = (2πmvr) / h = (2π × 6.0 × 10^24 kg × 3 × 10^4 m/s × 1.5 × 10^11 m) / (6.63 × 10^-34 Js) ≈ 2.55 × 10^74. This extremely large value of ‘n’ highlights that Bohr's model is not appropriate for macroscopic systems like the solar system. It was designed to model the behavior of electrons within atoms.</p> Signup and view all the answers

    Study Notes

    Atomic Structure

    • Atoms contain equal positive and negative charges
    • Thomson's model: Atom is a sphere of positive charge with electrons embedded
    • Rutherford's model: Atom has a small, dense, positive nucleus with electrons orbiting around it.
    • Rutherford's model had issues with atomic stability (electrons losing energy and spiraling into the nucleus).
    • Bohr model: Postulates a quantized model and stable orbits for the electrons in atoms (electron can only occupy certain energy levels)
    • Bohr model explained the discrete energy levels and emission/absorption spectra of hydrogen atoms but failed for multi-electron atoms
    • De Broglie's explanation: Explained the quantization of angular momentum; the electrons' wave nature forms standing waves.
    • Bohr's model was a stepping stone towards quantum mechanics

    Hydrogen Atom

    • First atomic model incorporating quantum ideas
    • Electrons exist in specific energy levels (stationary orbits, quantized states), and do not emit radiation while in these
    • When electron transitions between energy levels, photons are emitted or absorbed (frequencies of these photons relate to these transitions)
    • Orbital radii and energy are directly proportional to n²
    • Electrons in hydrogen's ground state: -13.6 eV; ionisation energy: +13.6 eV
    • Energy levels: progressively larger absolute value as n increases

    Rutherford's Experiment

    • Scattered alpha particles from a thin gold foil.
    • Most alpha particles passed straight through, some deflected at large angles.
    • This unexpected large-angle scattering suggested a small, dense, positively charged nucleus at the center of the atom.
    • The nucleus takes up a small fraction of the atom's total volume.
    • Most of the atom is empty space.

    Atomic Spectra

    • Characteristic spectrum for each element.
    • Emissions: Lines represent frequencies of emitted photons from excited electrons; atoms emit light at specific wavelengths.
    • Absorption: Dark lines on a continuous spectrum represent frequencies of absorbed photons (by atoms absorbing light at specific frequencies).

    Bohr Model Limitations

    • Applicable only to single-electron atoms (hydrogenic atoms)
    • Doesn't account for intensities of spectral lines (only frequencies)

    Energy Level Diagram

    • Shows relative energy levels of electrons
    • Higher energy levels are further away from the nucleus

    Additional Notes

    • The electron shells get progressively closer as they increase in energy level.
    • Electrons are in constant motion.
    • Electrons transition from one energy level to another by emitting or absorbing photons.
    • Quantum numbers and different levels of orbitals.

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    Description

    Explore the foundational concepts of atomic structure, including key models from Thomson to Bohr. This quiz covers the evolution of atomic theory and the quantum mechanics framework applied to the hydrogen atom. Test your understanding of how these models contribute to our knowledge of atomic behavior.

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