Solve Stopping Potential when 250 nm Light Hits Zinc Plate

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The discussion revolves around calculating the stopping potential when 250 nm light strikes a zinc plate, using the equation K = E - φ, where K is kinetic energy, E is the energy of the incident light, and φ is the work function. The user correctly derives the stopping potential formula, V = (hc/λ - φ)/q, and confirms that plugging in the values will yield the correct stopping potential. The conversation highlights that while the problem is framed within a quantum mechanics context, it primarily utilizes high school physics principles. Participants agree on the validity of the approach and clarify the educational purpose of including such problems in introductory courses. The solution process is validated, emphasizing the importance of understanding the underlying physics concepts.
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Homework Statement



I'm doing some practice problems for an introductory quantum mechanics course and am unsure whether or not I'm solving this problem properly - I need confirmation if I'm doing it right and help if I'm doing it wrong! :)

"What is the stopping potential when 250 nm light strikes a zinc plate?" (Chapter 3, #18 in Modern Physics 2nd ed. by Randy Harris)

Homework Equations



K = E - \varphi (where K is the kinetic energy, E is the energy of the incident light and \varphi is the work function)

This can be written as:

\frac{mv^2}{2} = \frac{hc}{\lambda} - \varphi (where m is the mass of a scattered electron, v is the speed of this electron, h is Planck's constant and c is the speed of light)

\frac{mv^2}{2} = qV (where q is the electron charge and V is the stopping potential)

h = 6.626 x 10^(-34) Js
c = 3 x 10^8 m/s
\varphi = 4.3 eV

The Attempt at a Solution



If my equations above are correct, I can write:

\frac{mv^2}{2} = \frac{hc}{\lambda} - \varphi = qV
\frac{hc}{\lambda} - \varphi = qV
V = \frac{\frac{hc}{\lambda} - \varphi}{q}

I can then simply plug in my values (remembering to either convert h in eV*s or \varphi into J) and this should give me the stopping potential, correct?
 
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Yes, that all looks good. No quantum mechanics in there, though; its all high school physics.
 
Thanks! And you're right, there isn't really any quantum mechanics here; it's just included in part of the course and its part of the introduction leading into the actual quantum mechanics.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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