L&T, 1..6
L&T, 1..1.2.4
Here we summarise the properties of the powers.
First of all the product of two powers,
{a}^{x}{a}^{y} = {a}^{x+y}\quad ,
| (2.1) |
e.g., {3}^{2}{3}^{6} = {3}^{8}, and {3}^{1∕2}{3}^{3∕2} = {3}^{2} (we see that x and y do not have to be integers (whole numbers)). Question: Evaluate {5}^{7∕10}{5}^{3∕10}.
If we take the power of a power, we multiply the exponents,
{
({a}^{x})}^{y} = {a}^{xy}
| (2.2) |
e.g., {({2}^{3})}^{2} = {8}^{2} = 64 = {2}^{3×2} = {2}^{6} = 64. This again works for x,y not integers. Question: Evaluate {2}^{1∕4}{4}^{3∕8}.
If the exponent is 1∕n we are taking the nth root of a,
{a}^{1∕n} = \root{n}\of{a},
| (2.3) |
e.g., {2}^{{1\over 2} } = \sqrt{2}, {2}^{{1\over 3} } = \root{3}\of{2}. If x = {a}^{{1\over n} } then {x}^{n} = a. This can be shown by taking both sides to the power n,
{x}^{n} ={ ({a}^{1∕n})}^{n} = {a}^{1} = a.
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The number n is often taken to be an integer, but it does not have to be. (E.g., {({3}^{1∕9.5})}^{9.5} = 3.)
If we take a number to the power zero, we find
{a}^{0} = 1\text{ for any }a > 0.
| (2.4) |
This follows from {a}^{0}{a}^{x} = {a}^{x+0} = {a}^{x}, and therefore {a}^{0} = 1. (Note that there is a slight problem with {0}^{0}: {0}^{x} = 0 for x > 0. One usually defines {0}^{0} = 1.)
If we take a number to a negative power, we write the result as a fraction involving a positive power,
{a}^{−x} = {1\over {
a}^{x}}
| (2.5) |
since {a}^{−x}{a}^{x} = {a}^{−x+x} = {a}^{0} = 1. Therefore {a}^{−x} = {1\over { a}^{x}}. E.g., {2}^{−1} = 1∕2.
Remember that
{a}^{x+y} = {a}^{x}{a}^{y}\quad \text{CORRECT!!!},
| (2.6) |
and not
{a}^{x+y}\mathrel{≠}{a}^{x} + {a}^{y}\quad \text{WRONG!!!}
| (2.7) |
As an example, {2}^{3+5} = {2}^{8} = 64, but {2}^{3} + {2}^{5} = 8 + 32 = 40.
L&T, 1..6.2
The exponential function is a special case of a power, where y = {e}^{x}, with e = 2.71828.... (Euler’s number). One also writes \mathop{exp}\nolimits (x) instead of {e}^{x}.
As we can see from Fig. 2.1, {e}^{x} is never less than 0 for any x. From the properties of powers we know that {e}^{−x} = {1\over { e}^{x}}. This function is also shown in Fig. 2.1, and is positive as well.
Differential (derivative w.r.t. x) of {e}^{x} is {e}^{x}, i.e.,
\class{boxed}{ {d{e}^{x}\over
dx} = {e}^{x}\quad . }
|
(This is the only function with the property that the derivative equals the function itself.)
If y = {e}^{ax} then {dy\over dx} = a{e}^{ax} (this is a form of the chain rule, which will be discussed later), e.g., if y = 3{e}^{7x} then {dy\over dx} = 3 × 7{e}^{7x} = 21{e}^{7x}.
Example 2.1:
Discuss exponential growth/decay.
Solution:
Exponential growth or decay is ruled by the form N(t) = {N}_{0}{e}^{at}. For a < 0 we have decay, for a > 0 we have growth. From the derivative, {dN\over dt} (t) = {N}_{0}a{e}^{at} = aN(t) we see that this arrises when the change in N is proportional to the number present. Examples are population growth, radioactive deay, ….
L&T, 1..6.3
L&T, 1..6.3.1
The inverse {f}^{−1} of a function f is defined such that if y = f(x), then x = {f}^{−1}(y).
A graph of the logarithm is shown in Fig. 2.2. If we swap the x and y axes, we recognise the exponential. Normally we use logs to base e (inverse of {e}^{x})- called natural logarithms, hence the name \mathop{ln}\nolimits (x), but we also write
\mathop{log}\nolimits (x) =\mathop{ ln}\nolimits (x)\quad .
|
L&T, 1..6.3.2
Just as y =\mathop{ ln}\nolimits x ⇒ x = {e}^{y} for the logarithm corresponding to base e (i.e., the inverse of {e}^{x}) for other bases we have y ={ \mathop{log}\nolimits }_{a}x ⇒ x = {a}^{y}. Here we use the notation that if we mean \mathop{log}\nolimits to base, say, 10 we write {\mathop{log}\nolimits }_{10}(x), i.e., if y ={\mathop{ log}\nolimits }_{10}(x), x = 1{0}^{y}.
It may help you to remember that a logarithm tries to extract a power from a number, e.g. the {\mathop{log}\nolimits }_{1}0 extract the power of 10 from a number.
Using this we can change from one base to another. Let y ={ \mathop{log}\nolimits }_{10}x, then x ={ 10}^{y}. Now let b =\mathop{ ln}\nolimits 10 (or \mathop{log}\nolimits 10), so 10 = {e}^{b}. Therefore x ={ ({e}^{b})}^{y} = {e}^{by}, so by =\mathop{ ln}\nolimits x, y = {\mathop{ln}\nolimits x\over b} = {\mathop{ln}\nolimits x\over \mathop{ln}\nolimits 10}. Hence {\mathop{log}\nolimits }_{10}x = {\mathop{ln}\nolimits x\over \mathop{ln}\nolimits 10}. Question: Determine α such that {\mathop{log}\nolimits }_{10}(x) = α{\mathop{log}\nolimits }_{2}(x).
If y =\mathop{ ln}\nolimits x then
\class{boxed}{ {dy\over
dx} = {1\over
x}\quad . }
|
(Remember that the differential of \mathop{ln}\nolimits x is 1∕x, not the integral! This is a common error!)
Using the fact that {e}^{{x}_{1}}{e}^{{x}_{2}} = {e}^{{x}_{1}+{x}_{2}}, i.e., the product of exponents is the exponent of the sum, we conclude that the inverse relation holds for logarithms. Thus, the logarithm of a product is the sum of the logarithms,
\mathop{ln}\nolimits ({y}_{1}{y}_{2}) =\mathop{ ln}\nolimits ({e}^{{x}_{1}
}{e}^{{x}_{2}
}) =\mathop{ ln}\nolimits {e}^{{x}_{1}+{x}_{2}
} = {x}_{1} + {x}_{2}.
|
Example 2.2:
The magnitude of a start is defined as m ={\mathop{ log}\nolimits }_{10}(I∕{I}_{0}). Explain how I changes if m increase by one unit.
Solution:
The new intensity satisfies {\mathop{log}\nolimits }_{10}({I}^{\text{new}}∕{I}_{0}) ={\mathop{ log}\nolimits }_{10}({I}^{\text{old}}∕{I}_{0}) + 1. Using the properties of the logarithms, we find that
Example 2.3:
An unresolved doube-star has magnitude 7. Find the individual magnitudes, assuming that both stars have the same one.
Solution:
Since intensities add up, we have 7 ={\mathop{ log}\nolimits }_{10}(2I∕{I}_{0}) ={\mathop{ log}\nolimits }_{10}(2) +{\mathop{ log}\nolimits }_{1}0(I∕{I}_{0}) ={\mathop{ log}\nolimits }_{10}(2) + m. Thus we conclude that m = 7 −{\mathop{ log}\nolimits }_{10}(2) = 6.69897.