14.11.2014 Views

Denition approach of learning new topics

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

26 4 DERIVATIVES<br />

seconds will travel 2t metres. So the function relating the time taken t to<br />

travel x distance is given by 5 x = 2t<br />

or x(t) = 2t<br />

So what is the rate <strong>of</strong> change <strong>of</strong> displacement with respect to time, between<br />

t = 1 and t = 2.<br />

We know that rate <strong>of</strong> change <strong>of</strong> displacement is ∆x<br />

∆t = x 2 − x 1<br />

= 4 − 2<br />

t 2 − t 1 2 − 1 =<br />

2. In physics, rate <strong>of</strong> change <strong>of</strong> diplacement is termed as velocity.<br />

Hence the average velocity is 2.<br />

What if we want to nd the instateneous velocity at t = 1. For that we<br />

need to get the secant at t = 1 which is a tangent. And we know that the<br />

tangent is the derivative. So the velocity at t = 1 is dx<br />

dt = d dt (2t) = 2<br />

2. A particle starts moving from a starting point A such that velocity at<br />

every point is given by v = 2t 3 where t is the time taken. Then how is<br />

acceleration related to velocity and time taken.<br />

v = 2t 3<br />

The rate <strong>of</strong> change <strong>of</strong> velocity is termed in physics as acceleration i.e.<br />

a = dv . Dierentiating we get,<br />

dt<br />

a = dv<br />

dt = d dt (2t3 ) = 2 d dt (t3 ) = 2 · 3t 2 = 6t 2<br />

4.5 Instantaneous rate <strong>of</strong> change[3]<br />

Now we know that average rate <strong>of</strong> change in the function y = f(x) is represented<br />

as ∆y and to get the instantaneous rate we use the limit <strong>of</strong> average<br />

∆x<br />

∆y<br />

lim<br />

∆x→0 ∆x<br />

5 Since x can be expressed in terms <strong>of</strong> variable t. Second notation describes that. We have<br />

see if a function f is expresses in terms <strong>of</strong> x then we write it as y = f(x).

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!