By now, students should appreciate the importance of placing units on quantities. This helps avoid errors such as using inches and feet for length in the same computation. Also, by canceling units in calculations, it is possible to determine the units of the answer, an obvious advantage for complex calculations where you could not expect to guess the units of the answer ahead of time. The real power of these methods will now be revealed to you. As the saying goes "you ain't seen nothing yet!"
1) Dimensions If a student were asked "what is money?", the answer "dollars" would be unsatisfactory; dollars is merely one particular example of money, and does not define what money actually is - a medium of exchange. Similarly, velocity is not well defined as ft/sec since this is only one example of a velocity Fundamentally, velocity is distance/time; in short hand V = D/t = Dt-1. We say that the dimensions of velocity are Dt-1. Similarly, the dimensions of acceleration are a = velocity/time = v/t = D/t/t = Dt-2. The dimensions of area are D2 , volume is D3. The dimensions of anything are the most basic quantities that can be used to express it. The four basic quantities of physics are:
2- time t
3- mass m
4- electric charge Q
Checking formulas is simple. You have seen that the formula for the distance traveled by an object accelerating from rest is D = 1/2at2 or is it D = 1/2a2t? Unlike the Columbus example, it is simple to select between the two possibilities. Any equation from physics is actually two equalities at once, numerical and also dimensional. That is, the dimensions of both sides of the equation must be equal. Lets examine both sides of each possibility and see how the dimensions work out:
This formula is possible. This is impossible
1) D = f (a, t) this merely says that the distance is a function of a,t
2) D = caxty c is a constant, x and y are exponents
whose value we seek to determine.
recall that the dimensions of acceleration are Dt-2
; substitute this for a.
3) D = c(Dt-2)xty
D = cDxt-2xty
D = cDxt-2x+y
4) Now there is a time variable on the right hand side of the equation but none on the left so we place to (which is 1) on the left hand side.
Dimensional analysis is a very powerful tool for physics which takes
time and practice to either master or fully appreciate. You will employ
it dozens of times in the rest of the course and should become quite expert
with the technique. The first example you try may be difficult but with
time you will see just how simple dimensional analysis is.
(1) Use dimensional reasoning to decide which of the following motion formulas could be correct, if any.
a) D = V2/a b)t =D/a
(2) The velocity reached after a period of acceleration from rest seems
related to the distance traveled and to the acceleration achieved. Use
dimensional analysis to discover the proportions.
Find a formula from the motion chapter that can be rearranged to support the result you got. __________ What is the value of the constant? _________________________
(3) The time for a single swing of a pendulum seems somehow related
to the acceleration of gravity, to the length of the pendulum, and possibly
to the mass m. Use dimensional analysis to derive an expression. (The acceleration
of gravity (called g) is dimensionally identical to any other acceleration.)
If you are really good, you can use dimensional analysis to show that the distance the pendulum swings sideways doesn't matter.
(4) The distance traveled by a body accelerating from rest seems related
to the acceleration of the body and to the velocity attained. Use dimensional
analysis to discover the proportions.
Find a formula from the motion chapter that can be rearranged to agree with your result. ______________
What is the constant c? _________________________
(5) Density can be defined various ways. For solid objects and liquids,
density is mass/volume, for wires etc. we have line density = mass/length
but for sheet metal and paper etc., we say area density = mass/area. What
are the dimensions of each type of density?
(6) An object thrown horizontally from a cliff or rooftop lands on the
ground below. There seems to be a relationship between the range
(our name for the distance the object travels sideways from the bottom
of cliff) and the velocity of throwing, the acceleration of gravity, and
the height of the cliff. Use dimensional analysis to derive the proportion
of range to velocity of throwing, acceleration of gravity, and cliff height.
if you find the algebra impossible to solve, then try treating distance
horizontal and distance vertical as different variables and try again.
Alternatively you can look back to your lab on the range of a projectile
and substitute the empirically found exponent for the range into this analysis.
(7) In a later chapter we will show that centripetal force (the force
that maintains objects traveling in a circle) is given as:
Centripetal Force = mV2 where r is the radius. What
are the dimensions of centripetal force?
r
(1) Only formula (a) is possible.
(2) Start with V = caxDy Since V is Dt-1
and a is Dt-2 we now have:
Dt-1 = c(Dt-2)xDy
from here we get Dt-1 = cDx t-2x
Dy = ct-2x Dx+y
___
__
1 = x + y and -1 = -2x. x= 1/2, y = 1/2.
The final result is thus V = ca 1/2 d1/2 = cÖ
ad . The c is actually Ö 2 .
(3) Start with t = cLxgymz then realize
that L is a distance and g, the acceleration of gravity, is merely acceleration
dimensionally. Thus we modify to get:
t = cDxaymz
___
This gives the result that t = cL1/2
g-1/2 = cÖ l/g The mass is irrelevant.
The ambitious student may want to include
the sideways swing in his analysis but finds that with two distance variables,
the
algebra can't be solved. However if sideways
motion is called Dhorizontal and the length and the D variable
in g is Dvertical,
then the problem vanishes. In other words
sideways swing = DH and length = DV and g = DVt-2
(4) Start with D = cVxay and end up with D =
cV2. The c turns out to be 1/2.
a
(5) Volume density is mD-3, area density is mD-2, line density is mD-l
(6) You start with Range = cVhoriz xgy Hz; Vhoriz = Dt-l, acceleration of gravity g is Dt-2 and Height is D.
Of course range R is also D.