I did not understand this derivative -- help please

  • Thread starter cemtu
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  • #1
cemtu
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Homework Statement:
Mathematical Methods in Physics
Relevant Equations:
Derivative
I have no idea how this derivative was taken.
 

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  • #2
It's wrong. ##N_{0}## is a constant (assuming the conventional interpretation of ##N_0## as the value of ##N## at ##t=0##). ##\frac{dN_0}{dt}## is always going to be ##0## and doesn't really make any sense. And to go one further, you still need to derive ##e^{-\lambda t}## wrt ##t##.
 
  • #3
cemtu
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dN0/dt = 2 is given thus N0 is 2t. There is no problem there sir.
 
  • #4
PeroK
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dN0/dt = 2 is given thus N0 is 2t. There is no problem there sir.
Your original post makes no sense. If you want any help you'll have to organise it into something meaningful.
 
  • #5
cemtu
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Okay right away.
 
  • #6
cemtu
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Your original post makes no sense. If you want any help you'll have to organise it into something meaningful.
I put the whole question and its solution.
 
  • #7
Are you sure you don't mean ##A_{0} = \left[-\frac{dN}{dt} \right]_{t=0} = 2##?

Of course, start off with the equation you wrote of ##N = N_{0}e^{-\lambda t}##. Then you can derive both sides with respect to ##t## to obtain a relation pertaining to the activities.

How would you derive the RHS wrt ##t##? Or perhaps more specifically, what can we do about the constant out the front?
 
  • #8
cemtu
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Are you sure you don't mean ##A_{0} = \left[-\frac{dN}{dt} \right]_{t=0} = 2##?

Of course, start off with the equation you wrote of ##N = N_{0}e^{-\lambda t}##. Then you can derive both sides with respect to ##t## to obtain a relation pertaining to the activities.

How would you derive the RHS wrt ##t##? Or perhaps more specifically, what can we do about the constant out the front?
I know how to derive however our professor just replaced N with dN/dt (LHS) and N0 with dN0/dt (RHS). I don't know how. He didnt took the derivative as the way you and I want.
 
  • #9
I know how to derive however our professor just replaced N with dN/dt (LHS) and N0 with dN0/dt (RHS). I don't know how. He didnt took the derivative as the way you and I want.

I can't speak for what your professor was trying to imply however I can say that ##\frac{dN_{0}}{dt}## is zero, as is the case for all constants. It's essentially a meaningless statement.

What do you get if you derive both sides of ##N = N_0 e^{-\lambda t}## with respect to ##t##?
 
  • #10
cemtu
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I can't speak for what your professor was trying to imply however I can say that ##\frac{dN_{0}}{dt}## is zero, as is the case for all constants. It's essentially a meaningless statement.

What do you get if you derive both sides of ##N = N_0 e^{-\lambda t}## with respect to ##t##?
Here
PHYSİCS.jpg
 
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  • #11
PeroK
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Here
I suspect this might be an initial value problem. But, you've misunderstood what's been given as initial values.

Without seeing the problem stated clearly, we are all just guessing.
 
  • #12
Here

You've done the differentiation right, ##\frac{dN}{dt} = -\lambda N_{0} e^{-\lambda t} \implies A = A_{0}e^{-\lambda t}## since ##A = \lambda N##.

You must stop using ##\frac{dN_{0}}{dt}##. It is wrong. I strongly suspect the intended meaning is the rate of change of ##N## at ##t=0##, however we might just denote this (negative) ##A_{0}## (or that more clunky expression in post #7).

You should be able to just plug in the ratio of the activities.
 
  • #13
cemtu
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You've done the differentiation right, ##\frac{dN}{dt} = -\lambda N_{0} e^{-\lambda t} \implies A = A_{0}e^{-\lambda t}## since ##A = \lambda N##.

You must stop using ##\frac{dN_{0}}{dt}##. It is wrong. I strongly suspect the intended meaning is the rate of change of ##N## at ##t=0##, however we might just denote this (negative) ##A_{0}## (or that more clunky expression in post #7).

You should be able to just plug in the ratio of the activities.
Sir, thank you.
 
  • #14
Sir, thank you.

You're welcome, though no need to call me 'sir', I haven't met the Queen yet!
 
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Without seeing the problem stated clearly, we are all just guessing.
This...
 

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