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My book has stumped me on something that I thought should be simple... perhaps I'm just not getting it.
Section - Constant Acceleration
It states the following:
"When acceleration is constant, the average acceleration and instantaneous acceleration are equal and we can write...
a = aavg = (v-v0)/(t-0)
Here v0 is the velocity at time t = 0 and v is the velocity at any later time t. We can recast this equation as:
v = v0 + at (Eq. 2-11)
As a check, note that this equation reduces to v = v0 for t = 0, as it must. As a further check, take the derivative of Eq. 2-11. Doing so yields dv/dt = a, which is the definition of a."
I'm not catching the last (bold) part. The derivative of equation 2-11 being equal to a.
When I work out the derivative (in my mind) is should work like this:
dv/dt = at
=a't + at'
=1(t) + a(1)
= t + a
My mind is leaning towards the idea that the book is trying say that dv/dt = a, at t = 0. Is that what the book is trying to tell me? Because I think I'm just confusing myself.
Any proof of this would probably help me out.
Thanks, prior!
Section - Constant Acceleration
It states the following:
"When acceleration is constant, the average acceleration and instantaneous acceleration are equal and we can write...
a = aavg = (v-v0)/(t-0)
Here v0 is the velocity at time t = 0 and v is the velocity at any later time t. We can recast this equation as:
v = v0 + at (Eq. 2-11)
As a check, note that this equation reduces to v = v0 for t = 0, as it must. As a further check, take the derivative of Eq. 2-11. Doing so yields dv/dt = a, which is the definition of a."
I'm not catching the last (bold) part. The derivative of equation 2-11 being equal to a.
When I work out the derivative (in my mind) is should work like this:
dv/dt = at
=a't + at'
=1(t) + a(1)
= t + a
My mind is leaning towards the idea that the book is trying say that dv/dt = a, at t = 0. Is that what the book is trying to tell me? Because I think I'm just confusing myself.
Any proof of this would probably help me out.
Thanks, prior!