Geology Reference
In-Depth Information
where ln is the natural logarithm, and
a δ t
=
at.
The integrations also yield constants of integration that can be combined into one, so
Eq. (A.3) becomes
ln( y )
=
at
+
c.
Taking the exponential of both sides, this becomes
y
=
exp( at
+
c )
=
exp( at )exp( c ) .
(A.4)
To evaluate the constant, we need to know a value of y at a particular time, t . Suppose
that, at time t
=
0, y has the value y 0 . Putting these values into Eq. (A.4) gives
y 0 =
exp(0) exp( c )
=
exp( c ) .
So Eq. (A.4) becomes
y
=
y 0 exp ( at ) .
(A.5)
This is the basic equation of exponential growth.
If it should happen that y is decreasing at a rate proportional to its size, the situation
can be covered by taking a to be negative. For example, sometimes a takes the form
a
=−
1 /τ.
The logic of solution follows exactly as that just described, and the solution takes the form
y
=
y 0 exp(
t/τ ) .
(A.6)
This is the basic equation of exponential decay, including radioactive decay.
We can also define a as 1 in Eq. (A.5). Then τ is a growth (or decay) time constant,
an 'e-folding' time. In other words, with each elapse of time t
=
τ , y increases by the
factor e
2.178. It is related to a half-life or a doubling time (depending on whether it is
decreasing or increasing). From Eq. (A.5), we can deduce that y will be twice y 0 when t
=
=
0.693 τ
ln(2) τ , where ln denotes a natural logarithm. Thus we can say that the doubling
time is τ 2 =
=
ln(2) τ . Similarly the half-life of decay in Eq. (A.6) is τ 1 / 2 =
ln(2) τ .
A.2 Post-glacial rebound
In Section 4.2, a relationship was derived between the depth, d , of a depression caused by
pre-existing ice and the rate of uplift, v , of the floor of the depression. Equation (4.8)
expresses the relationship as
μ
=
g ( ρ m
ρ w ) dR/v,
which we can rearrange as
v
=
g ( ρ m
ρ w ) Rd/μ.
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