The threshold frequency of a metal is \(f _0\) When the light of frequency \(2 f _0\) is incident on the metal plate, the maximum velocity of photoelectrons is \(v_1\) When the frequency of incident radiation is increased to \(5 f _0\), the maximum velocity of photoelectrons emitted is \(v_2\) The ratio of \(v_1\) to \(v_2\) is :
Remember Einstein’s photoelectric equation and how to relate the maximum kinetic energy of photoelectrons to their velocity.
\(\frac{v_1}{v_2}=\frac{1}{8}\)
\(\frac{v_1}{v_2}=\frac{1}{4}\)
\(\frac{v_1}{v_2}=\frac{1}{16}\)
\(\frac{v_1}{v_2}=\frac{1}{2}\)
Step 1: Apply Einstein’s Photoelectric Equation
Einstein’s photoelectric equation states:
\( K_{\text{max}} = hf - hf_0 \)
where \( K_{\text{max}} \) is the maximum kinetic energy of the emitted photoelectrons, \( h \) is Planck’s constant, \( f \) is the frequency of the incident light, and \( f_0 \) is the threshold frequency.
Step 2: Relate Kinetic Energy and Velocity
The maximum kinetic energy is also given by:
\( K_{\text{max}} = \frac{1}{2}mv^2 \)
where \( m \) is the mass of the electron and \( v \) is its velocity.
Step 3: Calculate \( v_1 \)
When \( f = 2f_0 \):
\( \frac{1}{2}mv_1^2 = h(2f_0) - hf_0 = hf_0 \)
Step 4: Calculate \( v_2 \)
When \( f = 5f_0 \):
\( \frac{1}{2}mv_2^2 = h(5f_0) - hf_0 = 4hf_0 \)
Step 5: Find the Ratio \( v_1 / v_2 \)
Dividing the equation for \( v_1^2 \) by the equation for \( v_2^2 \), we get:
\( \frac{\frac{1}{2}mv_1^2}{\frac{1}{2}mv_2^2} = \frac{hf_0}{4hf_0} \)
\( \frac{v_1^2}{v_2^2} = \frac{1}{4} \)
\( \frac{v_1}{v_2} = \frac{1}{2} \)
Conclusion: The ratio of \( v_1 \) to \( v_2 \) is \( \frac{1}{2} \) (Option 4).
A hydrogen atom consists of an electron revolving in a circular orbit of radius r with certain velocity v around a proton located at the nucleus of the atom. The electrostatic force of attraction between the revolving electron and the proton provides the requisite centripetal force to keep it in the orbit. According to Bohr’s model, an electron can revolve only in certain stable orbits. The angular momentum of the electron in these orbits is some integral multiple of \(\frac{h}{2π}\), where h is the Planck’s constant.
Ion | Q4+ | Xb+ | Yc+ | Zd+ |
---|---|---|---|---|
Radius (pm) | 53 | 66 | 40 | 100 |
Q4+, Xb+, Yc+, Zd+ are respectively
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
The atomic structure of an element refers to the constitution of its nucleus and the arrangement of the electrons around it. Primarily, the atomic structure of matter is made up of protons, electrons and neutrons.
Dalton proposed that every matter is composed of atoms that are indivisible and indestructible.
The following are the postulates of his theory:
Several atomic structures of an element can exist, which differ in the total number of nucleons.These variants of elements having a different nucleon number (also known as the mass number) are called isotopes of the element. Therefore, the isotopes of an element have the same number of protons but differ in the number of neutrons. For example, there exist three known naturally occurring isotopes of hydrogen, namely, protium, deuterium, and tritium.