de Broglie Wavelength in a Bohr Orbit

Physics · Dual Nature Of Radiation And Matter · NEET

In a Bohr orbit the electron behaves like a wave. A stable orbit exists only when a whole number of de Broglie wavelengths fits exactly around the circle, so 2*pi*r_n = n*lambda. This gives lambda = 2*pi*r_n / n. Memory hook: "the wave must bite its own tail" - the wave has to join up smoothly, so only whole waves (n = 1, 2, 3...) are allowed.
Standing electron wave: a whole number of wavelengths fits the orbitn = 4 (4 waves fit)n = 3 (3 waves fit)Condition2*pi*r_n = n*lambdalambda = 2*pi*r_n / nHydrogen: r_n = n^2 * a_0so lambda_n = 2*pi*n*a_0
A stable Bohr orbit exists only when a whole number n of de Broglie wavelengths joins up smoothly around the circle. From 2*pi*r_n = n*lambda you get lambda = 2*pi*r_n/n, and for hydrogen (r_n = n^2*a_0) this simplifies to lambda_n = 2*pi*n*a_0.

Your doubts, answered

Why does 2*pi*r = n*lambda in a Bohr orbit?

The electron in an orbit is a standing wave, not a moving ball. For a wave wrapped around a closed circle to be stable, its crest and trough must line up when it comes back to the start point. This only happens if the length of the orbit (the circumference 2*pi*r) is an exact whole-number multiple of the wavelength. So 2*pi*r_n = n*lambda, where n = 1, 2, 3... If it were not a whole number, the wave would overlap itself out of step and cancel (destructive interference), so no stable orbit forms.

How is 2*pi*r = n*lambda the same as Bohr's angular momentum rule?

Start from 2*pi*r = n*lambda and put lambda = h/p = h/(mv). Then 2*pi*r = n*h/(mv). Rearranging gives mvr = n*h/(2*pi). That is exactly Bohr's quantisation of angular momentum, L = n*h/(2*pi). So de Broglie's wave idea gives a physical reason WHY angular momentum is quantised - Bohr just assumed it, de Broglie explained it.

How many de Broglie wavelengths fit in the nth orbit?

Exactly n. In the first orbit (n = 1) one full wavelength fits around. In the second orbit (n = 2) two full wavelengths fit, and so on. So the number of wavelengths in an orbit equals its principal quantum number n. This is a very common NEET one-liner.

Does the de Broglie wavelength change from orbit to orbit?

Yes. lambda_n = 2*pi*r_n / n. For hydrogen r_n = n^2 * a_0, so lambda_n = 2*pi*(n^2*a_0)/n = 2*pi*n*a_0. This means lambda is directly proportional to n - the wavelength gets larger in higher orbits (lambda_2 = 2*lambda_1, lambda_3 = 3*lambda_1). Do not assume it stays constant.

How do I find the de Broglie wavelength for a given hydrogen state fast?

Use lambda_n = 2*pi*n*a_0 with a_0 = 0.053 nm. For n = 1: lambda = 2*pi*(1)(0.053) = 0.33 nm. For n = 2: lambda = 2*pi*(2)(0.053) = 0.67 nm. For n = 3: lambda = 2*pi*(3)(0.053) = 1.0 nm. This one shortcut answers the NEET 2025 question directly.

⚠️ The NEET trap
Using lambda = 2*pi*r_2 = 2*pi*(0.208 nm) = 1.31 nm, treating the circumference as one wavelength.
Two wavelengths fit in the n = 2 orbit, so 2*pi*r_2 = 2*lambda, giving lambda = 2*pi*(0.208)/2 = pi*(0.208) = 0.65 nm which is close to 0.67 nm. Always divide the circumference by n.
🧠 For n = 2, students find r_2 correctly but forget to divide by n.

Real NEET questions

NEET 2025

The de Broglie wavelength of an electron in the n = 2 state of the hydrogen atom is close to (Given Bohr radius a_0 = 0.053 nm):

A · 1.67 nm
B · 2.67 nm
C · 0.067 nm
D · 0.67 nm
Solution: Step 1: Use Bohr's condition that a whole number of wavelengths fits the orbit: 2*pi*r_n = n*lambda, so lambda = 2*pi*r_n / n. Step 2: For hydrogen the orbit radius is r_n = n^2 * a_0. For n = 2: r_2 = (2)^2 * 0.053 = 4 * 0.053 = 0.208 nm. Step 3: Substitute with n = 2: lambda = 2*pi*(0.208)/2 = pi*(0.208) = 3.14 * 0.208 = 0.65 nm. Step 4: This rounds to about 0.67 nm. Answer: (D) 0.67 nm. Shortcut: lambda_n = 2*pi*n*a_0 = 2*pi*(2)(0.053) = 0.67 nm directly.

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Frequently asked

What is the de Broglie wavelength in a Bohr orbit?

It is the wavelength of the electron treated as a wave in its orbit. For the nth orbit lambda_n = 2*pi*r_n / n, and for hydrogen this simplifies to lambda_n = 2*pi*n*a_0.

What is the condition for a stable (stationary) Bohr orbit?

A whole number of de Broglie wavelengths must fit exactly around the orbit: 2*pi*r_n = n*lambda, with n = 1, 2, 3... This makes the electron wave a stable standing wave.

How many wavelengths fit in the ground state (n = 1)?

Exactly one full de Broglie wavelength fits around the first orbit. In general n wavelengths fit in the nth orbit.

Is the de Broglie wavelength larger or smaller in higher orbits?

Larger. Since lambda_n = 2*pi*n*a_0, the wavelength grows in direct proportion to n, so the n = 3 wavelength is three times the n = 1 wavelength.

How does de Broglie explain Bohr's angular momentum quantisation?

Putting lambda = h/(mv) into 2*pi*r = n*lambda gives mvr = n*h/(2*pi). This is Bohr's rule L = n*h/(2*pi), so the wave picture provides the reason behind it.