The question
Question: find the Laplace transform of 1.
β{1} =
1 The idea
The Laplace transform turns a function of t into a function of s.
It is an integral, but we almost never work it out: we use a table made from it.
β{f(t)} = β« from 0 to β of e^(βst) f(t) dt
The table rows we need.
1 β 1s
2 Use the table
Each part by its row: 1 gives 1 over s.
β{1} = 1s
3 Check
Let's check: read the table backwards.
1/s comes from 1: the question.
Right!
backwards: 1s β 1
Let's look back.
First: the idea.
Then: use the table.
Last: check.
βΆ Watch it solved
The question
Question: find the Laplace transform of 3e^(2t) + 4.
β{3e^(2t) + 4} =
1 The idea
The Laplace transform turns a function of t into a function of s.
It is an integral, but we almost never work it out: we use a table made from it.
β{f(t)} = β« from 0 to β of e^(βst) f(t) dt
The table rows we need.
e^(at) β 1s β a
1 β 1s
2 Split it up
The transform of a sum is the sum of the transforms.
A number in front waits outside.
= 3β{e^(2t)} + 4β{1}
β{af + bg} = aβ{f} + bβ{g}
3 Use the table
Each part by its row: e^(2t) gives 1/(s β 2), 1 gives 1 over s.
= 3 Γ 1s β 2 + 4 Γ 1s
Careful!
e to the at gives s minus a.
Here a is 2, so it is s β 2.
Careful: not β{e^(2t)} = 1s + 2 β
4 Tidy up
Multiply the numbers: 3/(s β 2) + 4 over s.
= 3s β 2 + 4s
5 Check
Let's check: read the table backwards.
3/(s β 2) + 4/s comes from 3e^(2t) + 4: the question.
Right!
backwards: 3s β 2 + 4s β 3e^(2t) + 4
Let's look back.
First: the idea.
Then: split it up.
Then: use the table.
Then: tidy up.
Last: check.
βΆ Watch it solved
The question
Question: find the Laplace transform of e^(2t), from the definition.
β{e^(2t)} =
1 Use the definition
The definition: multiply by e to the minus st, and integrate from 0 to infinity.
β{f(t)} = β« from 0 to β of e^(βst) f(t) dt
Here f(t) is e^(2t).
β{e^(2t)} = β« from 0 to β of e^(βst)e^(2t) dt
Join the powers: βst + 2t is β(s β 2)t.
= β« from 0 to β of e^(β(s β 2)t) dt
e^(a) Γ e^(b) = e^(a + b)
2 Integrate
Integrate: divide by the number in front of t, which is β(s β 2).
= [βe^(β(s β 2)t)s β 2] from 0 to β
When t goes to infinity, e to a big minus power goes to 0.
That needs s > 2.
t β β: e^(β(s β 2)t) β 0 when s > 2
Careful!
If s is 2 or less, the power is not negative, and the integral never stops growing.
Careful: only for s > 2
3 Top minus bottom
At infinity: 0.
At 0: eβ° = 1, so β1/(s β 2).
Top minus bottom.
= 0 β (β1s β 2)
So β = 1/(s β 2), for s > 2.
= 1s β 2
4 Check
Let's check with the table row: e to the at gives 1/(s β a), with a = 2.
The same.
Right!
table: e^(at) β 1s β a, a = 2
Let's look back.
First: use the definition.
Then: integrate.
Then: top minus bottom.
Last: check.
βΆ Watch it solved