INTRODUCTION TO PHYSICS
1. Physics is a science. Science works according to the scientific method. The
scientific method accepts only reason, logic, and experimental evidence to tell
between what is scientifically correct and what is not. Scientists do not simply
believe – they test, and keep testing until satisfied. Just because some “big
scientist” says something is right, that thing does not become a fact of science.
Unless a discovery is repeatedly established in different laboratories at different
times by different people, or the same theoretical result is derived by clear use of
established rules, we do not accept it as a scientific discovery. The real strength of
science lies in the fact that it continually keeps challenging itself.
2. It is thought that the laws of physics do not change from place to place. This is
why experiments carried out in different countries by different scientists – of any
religion or race – have always led to the same results if the experiments have been
done honestly and correctly. We also think that the laws of physics today are the
same as they were in the past. Evidence, contained in the light that left distant
stars billions of years ago, strongly indicates that the laws operating at that time
were no different than those today. The spectra of different elements then and
now are impossible to tell apart, even though physicists have looked very
carefully.
3. This course will cover the following broad categories:
a) Classical Mechanics, which deals with the motion of bodies under the
action of forces. This is often called Newtonian mechanics as well.
b) Electromagnetism, whose objective is to study how charges behave under
the influence of electric and magnetic fields as well as understand how
charges can create these fields.
c) Thermal Physics, in which one studies the nature of heat and the changes
that the addition of heat brings about in matter.
d) Quantum Mechanics, which primarily deals with the physics of small
objects such as atoms, nuclei, quarks, etc. However, Quantum Mechanics
will be treated only briefly for lack of time.
4. Every physical quantity can be expressed in terms of three fundamental
dimensions: Mass (M), Length (L), Time (T). Some examples:
1
2
2
2 2
1 2
Speed
Acceleration
Force
Energy
Pressure
LT
LT
MLT
ML T
ML T
−
−
−
−
− −
You cannot add quantities that have different dimensions. So force can be added
to force, but force can never be added to energy, etc. A formula is definitely
wrong if the dimensions on the left and right sides of the equal sign are different.
5. Remember that any function f ( ) x takes as input a dimensionless number x and
outputs a quantity f (which may, or may not have a dimension). Take, for example,
the function f ( ) sin . θ = θ You know the expansion:
3 5
sin
3! 5!
θ θ θ θ = − + −⋅⋅⋅ If θ
had a dimension then you would be adding up quantities of different dimensions,
and that is not allowed.
6. Do not confuse units and dimensions. We can use different units to measure the
same physical quantity. So, for example, you can measure the mass in units of
kilograms, pounds, or even in sair and chatak! In this course we shall always use
the MKS or Metre-Kilogram-Second system. When you want to convert from one
hsystem to another, be methodical as in book
7. A good scientist first thinks of the larger picture and then of the finer details. So,
estimating orders of magnitude is extremely important. Students often make the
mistake of trying to get the decimal points right instead of the first digit – which
obviously matters the most! So if you are asked to calculate the height of some
building using some data and you come up with 0.301219 metres or 4.01219×106
metres, then the answer is plain nonsense even though you may have
miraculously got the last six digits right. Physics is commonsense first, so use
your intelligence before submitting any answer.
8. Always check your equations to see if they have the same dimensions on the left
side as on the right. So, for example, from this principle we can see the equation
2 2 2 2 22 v 2 is clearly wrong, whereas v 13 =+ =+ u at u a t could possibly be a
correct relation. (Here v and u are velocities, a is acceleration, and t is time.) Note
here that I use the word possibly because the dimensions on both sides match up
in this case.
9. Whenever you derive an equation that is a little complicated, see if you can find a
special limit where it becomes simple and transparent. So, sometimes it is helpful
to imagine that some quantity in it is very large or very small. Where possible,
make a “mental graph” so that you can picture an equation. So, for example, a
2 2 0 -(v-v ) /
formula for the distribution of molecular speeds in a
gas could look like (v) v . Even without
knowing the value of a you can immediately see that
a) (v) goes to zero fo
a f e
f
=
0
r large values of v, and v 0.
b) The maximum value of (v) occurs at v and the
function decreases on both side of this value.
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