@JohnRennie assuming the spiral in the question to be a disc of inner radius a and outer radius b won't change anything, right? It gets the right answer but I was wondering if there would be any issues in practical scenario
Thanks!! But if we do take a disc instead of such a spiral in real life then I'm thinking taking a disc in real life might reduce the resistance considerably and thus there would be more current in the disc, am I thinking it wrong?
I guess a solid disk of the same thickness of the wire would have more copper in it because the gaps between the wires would all be filled. To be a fair comparison you'd need to reduce the thickness of the disk so both the disk and the spiral had the same weight of copper.
And you'd need some way to induce a circular current in the disk.
Practically it would actually be quite difficult to compare the two.
We normally consider an idealised reversible process where the two phases are always in equilibrium. That means both the water and the ice have to be exactly at the melting point, and the transfer of heat from the water to the ice is infinitely slow.
In real life the water would have to be slightly above the melting point so there is a temperature difference between the water and the ice. Then heat flows from the water to the ice.
It's because we are considering a limit not a realistic system.
In real life there is some temperature difference ΔT i.e. the water is slightly hotter than the ice, and then there is a heat flow that is approximately proportional to the temperature difference: dQ/dt ∝ ΔT
So you are indeed going to end up with ice and water in equilibrium at 273K.
With problems like this it's hard to know in advance what the final state will be i.e. whether condensing then cooling the steam will produce enough heat to melt all the ice or not.
You just have to try the calculation to see what happens.
imgur.com/a/SaAwMXk | In this question, I can't do the third subpart. It says to find the variation of the refractive index required wrt time, but I think to get central maxima at O we only need one with a specific constant refractive index.
I have attached my work, and as all this variation with time in the refractive index of the medium is doing is linearly contracting the fringes, we need to get central maxima at O, which will not be affected by contractions.
specifically, $\mu_p = \frac{d}{p} sin\phi + 1$
The book's answer is $\mu_p = \mu_o + kt + \frac{d}{p}sin\phi$
Q: A solid sphere is in rotation about its polar axis ( z- axis) with angular accn= k(angular displacement) where when angular displacement=0, angular velocity= 0 at t=0 and motion was started by giving a very small push to the periphery of the sphere. A point p on the sphere is at 37 degree latitude from the center, what is the unit vector in the direction if acceleration of point P at the instant 'P' completes its first rotation?
I tried : P's radius for its circular motion in x-y plane is 4R/5. angular velocity * d/d(ang displacement) of angular velocity = k * angular displacement, so I integrated this on the RHL from 0 to 2pi and on the LHL from 0 to final angular velocity, I got Angular velocity final = (√k) * 2π
So acceleration vector = centripetal acceleration (I) + tangential acceleration (j) and substituted. The answer though has the tangential acceleration in the negative direction I.e out of the page, how is the direction realised ? The question doesnt mention if its clockwise or anticlockwise....?
To be precise the answer I get is (2π (î) + j)/√(4π²+1). The answer given is: (2π (î) - j)/ √(4π²+1).