Physics, asked by sorav2622333, 11 months ago

If force (F), velocity (u) and time (T) are taken
as fundamental quantities, then dimension of
length is​

Answers

Answered by Anonymous
46

Answer:

[ u T ]  

Explanation:  

\large \text{Let $L \propto F^a \ V^b \ T^c \ ...(i) $}\\\\\\\large \text{We know dimension of Force = $\left[MLT^{-2}\right]$}\\\\\\\large \text{Velocity = $\left[LT^{-1}\right]$}\\\\\\\large \text{Time= $\left[T^1 \right]$}}\\\\\\\large \text{We putting all values }\\\\\\\large \text{$\left[M^0LT^0\right]= k\left( \left[MLT^{-2}\right] \right )^a \left( \left[LT^{-1} \right] \right)^b\left(\left[T^1 \right]\right)^c$}

\large \text{$\left[M^0LT^0\right]= k\left( \left[M^\right] \right )^a \left( \left[L\right] \right)^{a+b}\left(\left[T\right]\right)^{-2a-b+c}$}

Now comparing on both side we have :  

a = 0  

a + b = 1

b = 1 - a

b = 1

-2 a - b + c = 0

- b + c = 0  

c = b  

c = 1  

Now put all these value in ( i ) we get

\large \text{$L \propto F^a \ V^b \ T^c \ ...(i)$}\\\\\\\large \text{$L= k \ F^0 \ V^1 \ T^{1} \ ..$}\\\\\\\large \text{$L= k \ VT$}\\\\\\\large \text{Given V = velocity = u}\\\\\\\large \text{So , we can write it as L = [ u T ]}

Thus , we get Dimension of Length is [ u T ] .


Tomboyish44: Great Answer!
Anonymous: Thank you : )
Answered by shadowsabers03
19

We're given that force (F), velocity (u) and time (T) are taken as fundamental quantities. We have to derive length (L) in terms of these three.

Well, a simple method is given below.

Among the given three, first we consider the derivation of a derived quantity in terms of the others, including L, in real situation.

In real situation, T is a fundamental quantity, so it can't be considered.

Consider F.

We know  [F]=[ma],\ \ \ [a]=\left[\dfrac{u}{T}\right]  and  [u]=\left[\dfrac{L}{T}\right]

So,  [F]=\left[\dfrac{mL}{T^2}\right]\ \implies\ [L]=\left[\dfrac{FT^2}{m}\right]

But this can't be accepted, because it's not given in the question that mass is taken as a fundamental quantity!

So this can't be taken.

Finally, consider u.

We had  [u]=\left[\dfrac{L}{T}\right]

This implies  [L]=[u\ T]

Well, this is enough!

Including F, we can rewrite it as,

\Large\boxed{[L]=F^0\ u^1\ T^1}


Tomboyish44: Great Answer!
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