Problem 21
Question
For a certain metal, \(v=2 v_{0}\) and the electrons come out with a maximum velocity of \(4 \times 10^{6} \mathrm{~ms}^{-1}\). If the value of \(v=5 v_{0}\), then maximum velocity of photelectrons will be (a) \(2 \times 10^{7} \mathrm{~ms}^{-1}\) (b) \(8 \times 10^{6} \mathrm{~ms}^{-1}\) (c) \(2 \times 10^{6} \mathrm{~ms}^{-1}\) (d) \(8 \times 10^{5} \mathrm{~ms}^{-1}\)
Step-by-Step Solution
Verified Answer
The maximum velocity of the photoelectrons is \(8 \times 10^6\) ms\(^{-1}\), option (b).
1Step 1: Understand the Photoelectric Effect Equation
The photoelectric effect equation relates the kinetic energy of ejected electrons to the energy of the incident light and the work function of the metal. It is given by \( KE_{ ext{max}} = h(v - v_0) \), where \( KE_{ ext{max}} = \frac{1}{2}mv^2 \), \( h \) is Planck's constant, \( v \) is the frequency of the incident light, \( v_0 \) is the threshold frequency, and \( v \) is the velocity of the electrons.
2Step 2: Convert Given Information into Equation Form
Given \( v = 2v_0 \), and the maximum velocity is \( 4 \times 10^6 \) ms\(^{-1}\). We use the photoelectric equation: \( \frac{1}{2}mv^2 = h(2v_0 - v_0) \). Similarly, if \( v = 5v_0 \), we need to find the new maximum velocity, which will be \( \frac{1}{2}mv'^2 = h(5v_0 - v_0) \).
3Step 3: Calculate Initial Kinetic Energy and Maximum Energy
For \( v = 2v_0 \), \( \frac{1}{2}m(4 \times 10^6)^2 = hv_0 \), providing the base kinetic energy. For \( v = 5v_0 \), \( \frac{1}{2}mv'^2 = 4hv_0 \), indicating the energy is now four times that initial value.
4Step 4: Express New Velocity in Terms of Known Values
Given \( \frac{1}{2}mv'^2 = 4 \times \frac{1}{2}m(4 \times 10^6)^2 \), solve for \( v' \): \( v'^2 = 4 \times (16 \times 10^{12}) \). Simplifying, \( v' = \sqrt{64 \times 10^{12}} = 8 \times 10^6 \) ms\(^{-1}\).
5Step 5: Identify the Correct Option
The maximum velocity of the photo-electrons when \( v = 5v_0 \) is \( 8 \times 10^6 \) ms\(^{-1}\), which matches option (b).
Key Concepts
Kinetic EnergyPlanck's ConstantThreshold Frequency
Kinetic Energy
In the context of the photoelectric effect, kinetic energy plays a crucial role in understanding how electrons behave when they are ejected from a material. When light strikes a metal surface, it transfers energy to the electrons. If this energy is enough to overcome the work function of the metal, electrons are ejected with some kinetic energy.
The kinetic energy of the ejected electrons in a photoelectric experiment is calculated using the equation: \[KE_{\text{max}} = \frac{1}{2}mv^2,\] where:
The kinetic energy of the ejected electrons in a photoelectric experiment is calculated using the equation: \[KE_{\text{max}} = \frac{1}{2}mv^2,\] where:
- \( KE_{\text{max}} \) is the maximum kinetic energy of the electron,
- \( m \) is the mass of the electron, and
- \( v \) is the velocity of the ejected electron.
Planck's Constant
Planck's constant \( h \) is a fundamental constant in physics that relates the energy of a photon to the frequency of the light. In the photoelectric effect, it helps us determine how much energy is being transferred from the light to the electron.
The photoelectric equation, which holds for the scenario where light of frequency \( v \) hits a metal, is given by: \[KE_{\text{max}} = h(v - v_0),\] where:
The photoelectric equation, which holds for the scenario where light of frequency \( v \) hits a metal, is given by: \[KE_{\text{max}} = h(v - v_0),\] where:
- \( h \) is Planck's constant,
- \( v \) is the frequency of the incident light, and
- \( v_0 \) is the threshold frequency of the metal.
Threshold Frequency
Threshold frequency \( v_0 \) is a vital concept when discussing the photoelectric effect as it represents the minimum frequency needed for electrons to be ejected from a metal surface.
The threshold frequency is the cut-off below which no electrons will be emitted, regardless of the light's intensity. It is a property unique to each material and influences whether electron ejection occurs. This can be seen in the equation for the photoelectric effect: \[KE_{\text{max}} = h(v - v_0).\]
The threshold frequency is the cut-off below which no electrons will be emitted, regardless of the light's intensity. It is a property unique to each material and influences whether electron ejection occurs. This can be seen in the equation for the photoelectric effect: \[KE_{\text{max}} = h(v - v_0).\]
- When \( v < v_0 \), \( KE_{\text{max}} \) becomes zero and no electron is ejected.
- When \( v \geq v_0 \), electrons are emitted and their kinetic energy can be calculated.
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