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Exploring Muscle Function: PNP Hydrolysis and ATP's Role, Study notes of Biology

The role of protein function in biological diversity and the use of atp as a molecular motor in muscle systems. Through the analysis of pnp hydrolysis, a model reaction similar to atp hydrolysis, we gain insights into the relevant bond changes and the concept of kinetic stability. The document also provides suggestions for textbook reading and homework exercises.

Typology: Study notes

2010/2011

Uploaded on 07/14/2011

ugochi141
ugochi141 🇺🇸

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Download Exploring Muscle Function: PNP Hydrolysis and ATP's Role and more Study notes Biology in PDF only on Docsity!

If you have purchased the custom 4 th edition of the textbook

you should have access to the full version online

Note :use BIO110OLEK to login

B110 Lecture 1 Summary Fall 2010

Find the most relevant textbook pages or figures in brackets [ ]

I. An understanding of protein [chpt. 3] function is critical in

explaining biological diversity, e.g. why skeletal muscle of some

animals are “stronger” or “faster” than others.

A. An experimental system can be used to demonstrate that

muscle [ fig. 46.17] uses a transduction device (molecular motor) to

convert some of the potential energy [ 27] of ATP to do

mechanical work

  1. System: isolated gastrocnemius muscle of a frog-- ~ 3 cm long

& 1 cm wide

  1. Environment: water @ 25

o

C + “salts”{we will not discuss yet

why “salts” are needed}

{ Note that it is important to define the relevant features of the

experimental system & environment

B110 Lecture 1 Summary (cont.)

IB. ALL experimental systems are designed to study change from

state 1, time = 0 to state 2, time = 0 + X

  1. e.g., When enough KCl is added to the environment of the muscle

system@ time = zero, the muscle length decreases ~ 30% ( from 3 to

2.1 cm length) in ~ 50 msec (state 2, time = 0 + 50 msec) {we will

not discuss yet how KCl causes this}

  1. e.g., When a mass is attached to the end of the muscle, a maximal

mass X is moved ~ 0.9cm

against the force of gravity -- by definition the experimental system

has done mechanical work.

PNP

PNP

CCCCCCONOO

POOO

What are the relevant

bond changes in

PNP hydrolysis?

What are the relevant

bond changes in

PNP hydrolysis?

C O P O

O

O

simpler model of PNP

C O P O

O

O PNP with Lewis bond model depicting

valence “bonding” electrons only for

C-O bond

PNP

PNP

What are the relevant bond changes in PNP hydrolysis?

C O P O

O

O

proton

proton

O

H

H

hydroxyl

ion

hydroxyl

ion

O

H

H

H 2 O

H 2 O

C O P O

O

O

O

H

H

A collision produces the

transition state

C O H O P O

O

O

PN H

PN

Pi

Pi

reactant

reactants

Some suggestions on how to get the most out

of textbook reading

Some suggestions on how to get the most out

of textbook reading

B110 Lecture 1 Summary Fall 2010

Find the most relevant textbook pages or figures in brackets [ ]

I. An understanding of protein [chpt. 3] function is critical in

explaining biological diversity, e.g. why skeletal muscle of some

animals are “stronger” or “faster” than others.

A. An experimental system can be used to demonstrate that

muscle [ fig. 46.17] uses a transduction device (molecular motor) to

convert some of the potential energy [ 27] of ATP to do

mechanical work

The author reminds you to use the “energy” concept in it

most narrow ( and useful sense) --please do so in BIO 110

The author reminds you to use the “energy” concept in it

most narrow ( and useful sense) --please do so in BIO 110

Text pg. 27

Text pg. 27

as kinetic energy (KE) = 1/2 mv

2

Reading

a textbook

Reading

a textbook

gastrocnemius muscle cell

system : state 1 time = 0

x

g

system : state 2

time = 0 + ~ 50 msec

0.9 cm

0.9 cm

x

g

myofibril

myofibril

After the experiment was done, you can now say the

myofibril state 1 system had “potential energy”

NOTE:

myofibril state 2 system

has less or even zero

“potential energy”

NOTE:

myofibril state 2 system

has less or even zero

“potential energy”

You can claim a system has “potential energy” only if you are

reasonably certain that work can be done by the system...

You can claim a system has “potential energy” only if you are

reasonably certain that work can be done by the system...

... or you are reasonably certain that the temperature of the state 2

environment will increase ( heat is “supplied, “released”, “generated”)

... or you are reasonably certain that the temperature of the state 2

environment will increase ( heat is “supplied, “released”, “generated”)

Let examine the potential energy of a “chemical” system

PNP + H 2 O PN + Pi

a “chemical system”

Keq >> 1

K eq

1

K eq << 1

K eq << 1

Would the temperature

of the environment

change with time?

Would the temperature

of the environment

change with time?

“perfect”

insulator

“perfect”

insulator

100% PNP

0 PN or Pi

state 1, time = 0

environment

environment

system

system

H 2 O @ 25

o

C

What if I gave BIO 110 students

tubes of PNP in water that

were perfectly insulated to

prevent heat loss?

Energy can be defined as the capacity of a system to

do work as it changes from state 1 to state 2. IF work

was done and/or the environmental temperature

increased the state 1 system had potential energy

Text pg. 27

Text pg. 27

More useful “verbal” definition of “energy”

More useful as it is easy to measure work done

and heat generated and report it in joules

More useful as it is easy to measure work done

and heat generated and report it in joules

B110 Lecture 1 Summary (cont.)

Preview of lecture 2 --> 3 :

I. Claim : Myosin proteins within muscle cells are the energy

transduction devices ( molecular motors) that produce the force

needed to do mechanical work

A. Testable Model : Myosin protein acts as an enzyme to reduce the

kinetic stability of ATP as an early step in the force generating

mechanism

net Work (J) of frog muscle system = force ( n) x displacement (m)

net Work (J) of frog muscle system = force ( n) x displacement (m)

Measured maximal force generated by a frog gastrocnemius muscle ~ 0.5 n

Measured maximal force generated by a frog gastrocnemius muscle ~ 0.5 n

gastrocnemius muscle

system : state 1 time = 0

v

kg

system : state 2

time = 0 + ~ 50 msec

1.0 cm

1.0 cm

v

kg

frog

gastrocnemius

muscle

frog

gastrocnemius

muscle

net Work (J) = (0.5 n) x ( 0.01 m) = 0.005 J

net Work (J) = (0.5 n) x ( 0.01 m) = 0.005 J

What is the maximum theoretical mass ( X )

the muscle can lift against gravity?

What is the maximum theoretical mass ( X )

the muscle can lift against gravity?

1.0 cm

1.0 cm

v

kg

What is the maximum theoretical mass ( v )

the muscle can lift against gravity?

What is the maximum theoretical mass ( v )

the muscle can lift against gravity?

measured Work (J) of frog muscle system

= 0.5 ( n) x 0.01 (m) = 0.005 J

measured Work (J) of frog muscle system

= 0.5 ( n) x 0.01 (m) = 0.005 J

Work (J) = mass (kg) x acceleration (m/s

2 ) x displacement (m)

0.005 J frog muscle Work = ( v mass in kg) x ( 10 m/s

2 ) x 0.01 (m)

acceleration displacement

0.005 J frog muscle Work = ( v mass in kg) x ( 0.1)

0.005 J frog muscle Work = v mass in kg

= 0.05 kg ( 50 g)

= 0.05 kg ( 50 g)