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Transfer Function
SUMMER SCHOOL
Physical Process
Mathematical Modeling
Using the Newton Laws, we have:
ma t + 𝑏𝑣(𝑑) + π‘˜π‘₯(𝑑) = F(t)
Now, we know that:
𝑣(𝑑) =
β…†π‘₯
ⅆ𝑑
= π‘₯(t) and π‘Ž 𝑑 =
β…†2 π‘₯
ⅆ𝑑2 = π‘₯(t)
Then we have:
π‘š π‘₯ 𝑑 + 𝑏 π‘₯ 𝑑 + π‘˜π‘₯ 𝑑 = 𝐹 𝑑
Now we solve for x to see the evolution of the system in time
Convolution
It is a mathematical operation between two signals in order to get a third signal.
S - Plane
Laplace Theorem do the conversion between Time - Domain and S – Plane
Weight function vs Transfer Function
h(t) -> Weight Function (system function represented in Time - Domain)
H(s) -> Transfer Function (system function represented in Frequency - Domain)
Example
TF for our Physical System
Differential equation from our example:
π‘š π‘₯ 𝑑 + 𝑏 π‘₯ 𝑑 + π‘˜π‘₯ 𝑑 = 𝐹 𝑑
After we apply Laplace Transform, becomes:
π‘šπ‘ 2 + 𝑏𝑠 + π‘˜ 𝑋 𝑠 = 𝐹 𝑠
Thus we get:
𝐻 𝑠 =
𝑋(𝑠)
𝐹(𝑠)
=
1
π‘šπ‘ 2 + 𝑏𝑠 + π‘˜
Where
H(s) -> Transfer Function for our Physical System
Questions?

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Transfer Function

  • 3. Mathematical Modeling Using the Newton Laws, we have: ma t + 𝑏𝑣(𝑑) + π‘˜π‘₯(𝑑) = F(t) Now, we know that: 𝑣(𝑑) = β…†π‘₯ ⅆ𝑑 = π‘₯(t) and π‘Ž 𝑑 = β…†2 π‘₯ ⅆ𝑑2 = π‘₯(t) Then we have: π‘š π‘₯ 𝑑 + 𝑏 π‘₯ 𝑑 + π‘˜π‘₯ 𝑑 = 𝐹 𝑑 Now we solve for x to see the evolution of the system in time
  • 4. Convolution It is a mathematical operation between two signals in order to get a third signal.
  • 5. S - Plane Laplace Theorem do the conversion between Time - Domain and S – Plane
  • 6. Weight function vs Transfer Function h(t) -> Weight Function (system function represented in Time - Domain) H(s) -> Transfer Function (system function represented in Frequency - Domain)
  • 8. TF for our Physical System Differential equation from our example: π‘š π‘₯ 𝑑 + 𝑏 π‘₯ 𝑑 + π‘˜π‘₯ 𝑑 = 𝐹 𝑑 After we apply Laplace Transform, becomes: π‘šπ‘ 2 + 𝑏𝑠 + π‘˜ 𝑋 𝑠 = 𝐹 𝑠 Thus we get: 𝐻 𝑠 = 𝑋(𝑠) 𝐹(𝑠) = 1 π‘šπ‘ 2 + 𝑏𝑠 + π‘˜ Where H(s) -> Transfer Function for our Physical System