Suppose quantity s is a length and quantity t is a time. Suppose the quantities v and a are defined by v = ds/dt and a = dv/dt. (a) What is the dimension of v? (b) What is the dimension of the quantity a? What are the dimensions of (c) ∫vdt,(d) ∫adt,and (e) da/dt?

Respuesta :

Answer:

a) [tex] v = \frac{[L]}{[T]} = LT^{-1}[/tex]

b) [tex] a = \frac{[L}{T}^{-1}]}{{T}}= L T^{-1} T^{-1}= L T^{-2}[/tex]

c) [tex] \int v dt = s(t) = [L]=L[/tex]

d) [tex] \int a dt = v(t) = [L][T]^{-1}=LT^{-1}[/tex]

e) [tex] \frac{da}{dt}= \frac{[L][T]^{-2}}{T} = [L][T]^{-2} [T]^{-1} = LT^{-3}[/tex]

Step-by-step explanation:

Let define some notation:

[L]= represent longitude , [T] =represent time

And we have defined:

s(t) a position function

[tex] v = \frac{ds}{dt}[/tex]

[tex] a= \frac{dv}{dt}[/tex]

Part a

If we do the dimensional analysis for v we got:

[tex] v = \frac{[L]}{[T]} = LT^{-1}[/tex]

Part b

For the acceleration we can use the result obtained from part a and we got:

[tex] a = \frac{[L}{T}^{-1}]}{{T}}= L T^{-1} T^{-1}= L T^{-2}[/tex]

Part c

From definition if we do the integral of the velocity respect to t we got the position:

[tex] \int v dt = s(t)[/tex]

And the dimensional analysis for the position is:

[tex] \int v dt = s(t) = [L]=L[/tex]

Part d

The integral for the acceleration respect to the time is the velocity:

[tex] \int a dt = v(t)[/tex]

And the dimensional analysis for the position is:

[tex] \int a dt = v(t) = [L][T]^{-1}=LT^{-1}[/tex]

Part e

If we take the derivate respect to the acceleration and we want to find the dimensional analysis for this case we got:

[tex] \frac{da}{dt}= \frac{[L][T]^{-2}}{T} = [L][T]^{-2} [T]^{-1} = LT^{-3}[/tex]

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