Canonical protein dynamics

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Canonical protein dynamics. Flowchart. Differential equation. Solution. f. 0. Physical picture of protein translation and degradation. No degradation for this protein. No translations. 10. 0. 11. 1. 12. 2. 13. 3. 14. 4. 15. 5. 16. 6. 17. 7. 18. 8. 19. 9. +. +. +. - PowerPoint PPT Presentation

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Canonical protein dynamics

1

Differential equationFlowchart

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

𝛽𝛼

π‘₯ (𝑑 )

𝑑0

Solution

2

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

No translations

Physical picture of protein translation and degradation

No degradation for this protein

+No

chan

ge

Physical picture of protein translation and degradation

3

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

Chance translation

+

+

Physical picture of protein translation and degradation

4

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

No

chan

ge

Neglecting to roll dice on this freshly

generated protein.

+

Physical picture of protein translation and degradation

5

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+N

o ch

ange

+

Physical picture of protein translation and degradation

6

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

Physical picture of protein translation and degradation

7

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

No

chan

ge

Rolled dice for protein that was

already degraded!

+

Physical picture of protein translation and degradation

8

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

Physical picture of protein translation and degradation

9

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

Physical picture of protein translation and degradation

10

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

Chance translation

+

Physical picture of protein translation and degradation

11

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

+

Physical picture of protein translation and degradation

12

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

+

Physical picture of protein translation and degradation

17

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

+

Physical picture of protein translation and degradation

18

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ + +

+

+

Chance translation

+

Physical picture of protein translation and degradation

19

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ + +

+

+

+

Physical picture of protein translation and degradation

20

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ + +

+

+

+

Physical picture of protein translation and degradation

21

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ + +

+

+

+

Physical picture of protein translation and degradation

22

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

+

βˆ† 𝑑

Between times and

β‰…2degradations

(20 time steps ) (28 proteins )(ΒΏ time steps ) (ΒΏ proteins )Proteins lost

β‰…3 translations20 time steps

(ΒΏ time steps )Proteins added β‰… π›½βˆ† 𝑑

β‰… π›Όβˆ† 𝑑 π‘₯ (𝑑 0 )π‘₯ (𝑑 0+βˆ†π‘‘ )β‰… π‘₯ (𝑑 0 )+π›½βˆ† π‘‘βˆ’π›Όβˆ† 𝑑 π‘₯ (𝑑 0 )

π‘₯ (𝑑 0+βˆ†π‘‘ )βˆ’π‘₯ (𝑑 0 )β‰… π›½βˆ† π‘‘βˆ’π›Όβˆ† 𝑑 π‘₯ (𝑑 0 )

𝑑π‘₯𝑑𝑑 |𝑑=𝑑 0β‰…

π‘₯ (𝑑0+βˆ† 𝑑 )βˆ’π‘₯ (𝑑0 )βˆ† 𝑑

β‰… π›½βˆ’π›Ό π‘₯ ( 𝑑0 )

𝑑 0 +

Physical picture of protein translation and degradation

23

𝑑 (𝜏𝐷𝐼𝐢𝐸 )2 3 4 5 6 7 8 90 1 12 13 14 15 16 17 18 1910 11 20

Note: Proteins can be distinguished by momentary distortions.

+ +

+

+

+

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯

+

STOPLimitation!!! (But we all do it this it this way)

x (# proteins)

28

29

30

Realistic trajectory

Unrealistically smooth trajectory

f𝛽 𝛼

π‘₯

Canonical protein dynamics

24

Differential equationFlowchart

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

𝛽𝛼

π‘₯ (𝑑 )

𝑑0

Solution

𝛽𝛼

Time-course and rise time

25

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

Declare initial condition, for example, β€œstart at time 0 with no protein”

π‘₯ (0 )=0

Look for possible steady states

0=𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯𝑆𝑇

π‘₯ (𝑑 )

𝑑0

π‘₯𝑆𝑇=𝛽𝛼

Estimate some slopes

Time-course and rise time

26

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

π‘₯ (𝑑 )

𝑑

0

𝛽𝛼

𝑑π‘₯𝑑𝑑

=𝛼 ( π›½π›Όβˆ’π‘₯ )𝑠 (π‘₯ )

𝑠 (π‘₯ )=βˆ’π‘₯+𝛽𝛼

𝑠 (π‘₯ (0 ) )= 𝛽𝛼

𝑠 (π‘₯𝑆𝑇 )=βˆ’ 𝛽𝛼 +𝛽𝛼

=0

𝑑 𝑠𝑑𝑑

=𝑑𝑠𝑑π‘₯

𝑑π‘₯𝑑 𝑑

𝑑 𝑠𝑑𝑑

= 𝑑𝑑π‘₯ (βˆ’ π‘₯+ 𝛽

𝛼 ) 𝑑π‘₯𝑑𝑑

βˆ’π‘‘π‘ π‘‘ 𝑑

=𝛼 𝑠

βˆ«π‘‘=0

𝑑 𝑓1𝑠𝑑 𝑠𝑑𝑑

𝑑𝑑=βˆ’π›Ό βˆ«π‘‘=0

𝑑 𝑓

𝑑𝑑

βˆ«π‘ =𝑠 (π‘₯ (0 ))

𝑠 ( π‘₯ (𝑑 𝑓 ) )1𝑠𝑑 𝑠=βˆ’π›Ό ∫

𝑑=0

𝑑 𝑓

𝑑𝑑

𝑑 𝑠𝑑𝑑

=βˆ’π‘‘π‘₯𝑑𝑑

Time-course and rise time

27

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

π‘₯ (𝑑 )

𝑑

0

𝛽𝛼

𝑠 (π‘₯ )=βˆ’π‘₯+𝛽𝛼

𝑠 (π‘₯ (0 ) )= 𝛽𝛼

𝑠 (π‘₯𝑆𝑇 )=βˆ’ 𝛽𝛼 +𝛽𝛼

=0

𝑑 𝑠𝑑𝑑

=𝑑𝑠𝑑π‘₯

𝑑π‘₯𝑑 𝑑

𝑑 𝑠𝑑𝑑

= 𝑑𝑑π‘₯ (βˆ’ π‘₯+ 𝛽

𝛼 ) 𝑑π‘₯𝑑𝑑

βˆ«π‘ =𝑠 (π‘₯ (0 ))

𝑠 ( π‘₯ (𝑑 𝑓 ) )1𝑠𝑑 𝑠=βˆ’π›Ό ∫

𝑑=0

𝑑 𝑓

𝑑𝑑

ln (𝑠 (π‘₯ ( 𝑑 𝑓 )) )βˆ’ ln( 𝛽𝛼 )=βˆ’π›Ό [𝑑 𝑓 βˆ’0 ]

𝑑 𝑠𝑑𝑑

=βˆ’π‘‘π‘₯𝑑𝑑

ln ( 𝑠 (π‘₯ (𝑑 𝑓 ) )𝛽𝛼 )=βˆ’π›Όπ‘‘ 𝑓𝑠 (π‘₯ (𝑑 𝑓 ) )

𝛽𝛼

=π‘’βˆ’π›Όπ‘‘ 𝑓

𝑠=π›½π›Όπ‘’βˆ’π›Όπ‘‘ 𝑓

𝑇 12

Time-course and rise time

28

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

π‘₯ (𝑑 )

𝑑0

𝑠=π›½π›Όπ‘’βˆ’π›Όπ‘‘ 𝑓

𝛽2𝛼

𝛽𝛼

𝛽2𝛼

𝛽𝛼

𝛽2𝛼

𝛽𝛼

𝛽2𝛼

𝛽𝛼

𝛽2𝛼

𝛽𝛼

𝑇 12

=ln (2 )𝛼

STOPShow

𝑇 12

𝑇 12

𝑇 12

𝑇 12

𝑇 12

𝛽2𝛼

Time-course and rise time

29

𝑑π‘₯𝑑𝑑

=π›½βˆ’π›Ό π‘₯f

𝛽 𝛼π‘₯

π‘₯ (𝑑 )

𝑑0

𝑠=π›½π›Όπ‘’βˆ’π›Όπ‘‘ 𝑓

𝛽𝛼

𝑇 12

=ln (2 )𝛼