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The only element in the hydrogen atom r...

The only element in the hydrogen atom resides under ordinary condition on the first orbit .When energy is supplied the element move to hjgher energy ornbit depending on the lower of energy absioerbed .When this electron to may of the electron return to any of the lower orbits, it emit energy Lyman series is formed when the electron to the lowest orbit white Balmer series ids formed when the electron returns to the second orbit similar Paschen Brackett, and Pfund series are formed when electron return to the third fourth , and fifth arbit from highest energy orbits, respectively
Maximum number of liner produced is equal when as electron jumps from nth level to ground level is equal to `(n(n - 1))/(2)`If teh electron comes back from the energy level having energy `E_(2)` to the energy level having energy `E_(1)` then the difference may be expresent in terms of energy of photon as `E_(2) - E_(1) = Delta E, lambda = hc//Delta E` Since h and c are constants `Delta E` coresponding to definite energy , thus , each transition from one energy level to unother will produce a light of definite wavelem=ngth .This isd actually observed as a line in the spectrum of hydrogen atom Wave number of line is given by the formula `bar v = RZ^(2)((1)/(n_(1)^(2))- (1)/(n_(12)^(2)))`Where R is a Rydherg constant
Its a single isolated atom, an electrons make transition from fifth excited state is second thern maximum number of different type of photon observed is

A

3

B

4

C

6

D

15

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To solve the problem, we need to determine the maximum number of different types of photons emitted when an electron transitions from the fifth excited state to the second excited state in a hydrogen atom. ### Step-by-Step Solution: 1. **Identify the Energy Levels**: - The fifth excited state corresponds to \( n = 6 \) (since the ground state is \( n = 1 \)). - The second excited state corresponds to \( n = 3 \). 2. **Determine the Transition Path**: - The electron will transition from \( n = 6 \) to \( n = 3 \). - During this transition, the electron can pass through the intermediate energy levels, which are \( n = 5 \), \( n = 4 \), and \( n = 3 \). 3. **Count the Transitions**: - The possible transitions are: - From \( n = 6 \) to \( n = 5 \) - From \( n = 5 \) to \( n = 4 \) - From \( n = 4 \) to \( n = 3 \) - Each transition corresponds to the emission of a photon. 4. **Calculate the Number of Different Photons**: - Each transition can emit a different photon. Therefore, the total number of different types of photons emitted during these transitions is equal to the number of transitions: - Transition 1: \( n = 6 \) to \( n = 5 \) (1 photon) - Transition 2: \( n = 5 \) to \( n = 4 \) (1 photon) - Transition 3: \( n = 4 \) to \( n = 3 \) (1 photon) - Thus, the total number of different types of photons emitted is \( 3 \). ### Final Answer: The maximum number of different types of photons observed when the electron transitions from the fifth excited state to the second excited state is **3**. ---

To solve the problem, we need to determine the maximum number of different types of photons emitted when an electron transitions from the fifth excited state to the second excited state in a hydrogen atom. ### Step-by-Step Solution: 1. **Identify the Energy Levels**: - The fifth excited state corresponds to \( n = 6 \) (since the ground state is \( n = 1 \)). - The second excited state corresponds to \( n = 3 \). ...
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The only element in the hydrogen atom resides under ordinary condition on the first orbit .When energy is supplied the element move to hjgher energy ornbit depending on the lower of energy absioerbed .When this electron to may of the electron return to any of the lower orbits, it emit energy Lyman series is formed when the electron to the lowest orbit white Balmer series ids formed when the electron returns to the second orbit similar Paschen Brackett, and Pfund series are formed when electron return to the third fourth , and fifth arbit from highest energy orbits, respectively Maximum number of liner produced is equal when as electron jumps from nth level to ground level is equal to (n(n - 1))/(2) If teh electron comes back from the energy level having energy E_(2) to the energy level having energy E_(1) then the difference may be expresent in terms of energy of photon as E_(2) - E_(1) = Delta E, lambda = hc//Delta E Since h and c are constants Delta E coresponding to definite energy , thus , each transition from one energy level to unother will produce a light of definite wavelem=ngth .This isd actually observed as a line in the spectrum of hydrogen atom Wave number of line is given by the formula bar v = RZ^(2)((1)/(n_(1)^(2))- (1)/(n_(12)^(2))) Where R is a Rydherg constant The difference in the wavelength of the second line is Lyman series and last line of breaker series is a hydrogen sample is

The only element in the hydrogen atom resides under ordinary condition on the first orbit .When energy is supplied the element move to hjgher energy ornbit depending on the lower of energy absioerbed .When this electron to may of the electron return to any of the lower orbits, it emit energy Lyman series is formed when the electron to the lowest orbit white Balmer series ids formed when the electron returns to the second orbit similar Paschen Brackett, and Pfund series are formed when electron return to the third fourth , and fifth arbit from highest energy orbits, respectively Maximum number of liner produced is equal when as electron jumps from nth level to ground level is equal to (n(n - 1))/(2) If teh electron comes back from the energy level having energy E_(2) to the energy level having energy E_(1) then the difference may be expresent in terms of energy of photon as E_(2) - E_(1) = Delta E, lambda = hc//Delta E Since h and c are constants Delta E coresponding to definite energy , thus , each transition from one energy level to unother will produce a light of definite wavelem=ngth .This isd actually observed as a line in the spectrum of hydrogen atom Wave number of line is given by the formula bar v = RZ^(2)((1)/(n_(1)^(2))- (1)/(n_(12)^(2))) Where R is a Rydherg constant If the ionisation potential for hydrogen -like atom in a sample is 122.4 V then the series limit of the paschen series for this atom is

The only element in the hydrogen atom resides under ordinary condition on the first orbit .When energy is supplied the element move to hjgher energy ornbit depending on the lower of energy absioerbed .When this electron to may of the electron return to any of the lower orbits, it emit energy Lyman series is formed when the electron to the lowest orbit white Balmer series ids formed when the electron returns to the second orbit similar Paschen Brackett, and Pfund series are formed when electron return to the third fourth , and fifth arbit from highest energy orbits, respectively Maximum number of liner produced is equal when as electron jumps from nth level to ground level is equal to (n(n - 1))/(2) If teh electron comes back from the energy level having energy E_(2) to the energy level having energy E_(1) then the difference may be expresent in terms of energy of photon as E_(2) - E_(1) = Delta E, lambda = hc//Delta E Since h and c are constants Delta E coresponding to definite energy , thus , each transition from one energy level to unother will produce a light of definite wavelem=ngth .This isd actually observed as a line in the spectrum of hydrogen atom Wave number of line is given by the formula bar v = RZ^(2)((1)/(n_(1)^(2))- (1)/(n_(12)^(2))) Where R is a Rydherg constant The wave number of electromagnetic radiation emitted during the transition of electron in between the two levels of Li^(2+) ion whose pricipal quantum numbner sum is 4 and difference is 2 is

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