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Learn it your way
A short class with Sarah and her students. The other ways are under More.
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You have just breathed in an oxygen molecule. It is now in an alveolus. Where does it go next?
Across the wall of the alveolus and into a capillary.
How many cell layers does it cross?
Two: the alveolar wall and the capillary wall, each just one flattened cell thick.
Right. Then it diffuses into a red blood cell and joins haemoglobin. Why does it move into the blood at all?
Because the blood arriving at the lungs has less oxygen than the air in the alveolus.
Exactly: from high concentration to low, with no energy needed. That is diffusion.
If oxygen keeps moving into the blood, shouldn't the two sides soon become equal and diffusion stop?
Not if the blood keeps moving away and new blood arrives.
Good, that's blood flow. What else helps?
Breathing, which keeps bringing fresh air into the alveoli.
And haemoglobin plays a clever part. Once oxygen binds to it, the free oxygen inside the cell stays low.
So more oxygen keeps diffusing in, as if it were filling a sponge rather than a glass.
A great way to picture it.
Your blood now reaches a leg muscle during a run. Which way does oxygen diffuse here?
Out of the blood and into the muscle cells, because they are using it up in respiration.
Yes, the gradient is reversed. And carbon dioxide?
It goes the other way, from the muscle cells into the blood.
Now, a disease makes the barrier in the lungs twice as thick. What happens to the rate of diffusion?
It halves, because the oxygen has twice as far to go.
Exactly. Surface area, concentration difference and thickness all control the rate.
Oxygen crosses the alveolar wall and the capillary wall, then enters a red blood cell and binds to haemoglobin.
Oxygen moves because the alveolar air holds more oxygen than the blood arriving at the lungs.
Breathing, blood flow and haemoglobin keep the concentration difference large.
Where cells use oxygen, it diffuses out of the blood; carbon dioxide diffuses the other way.
Surface area, concentration difference and barrier thickness together set the rate of diffusion.
During a deep breath, oxygen diffuses from alveolar air at about 100 mmHg into blood arriving at about 40 mmHg, until the blood leaving the lungs is almost as rich in oxygen as the air.
During a sprint, a leg muscle uses oxygen so fast that oxygen diffuses out of the passing red blood cells into the muscle cells, while carbon dioxide diffuses into the blood.
A mountaineer at high altitude breathes air with less oxygen, so the concentration difference across the alveolar wall is smaller and oxygen enters the blood more slowly.
High to low, oxygen goes; lungs to blood, then out to toes.
An oxygen molecule leaves a crowded alveolus, slips through two thin curtains into a red blood cell, rides the haemoglobin taxi to a busy leg muscle, and hops off where oxygen is scarce.
Surface, Steepness, Short distance: the three S's of fast diffusion.
A.C.R.H. - Alveolus, Capillary, Red blood cell, Haemoglobin: the oxygen's route into the blood.
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Which two cell layers does oxygen cross to get from an alveolus into the blood?
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Why does oxygen diffuse into the blood in the lungs?
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How does haemoglobin help keep the gradient steep?
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Why does oxygen leave the blood in a working muscle?
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What happens to the rate of diffusion if the barrier becomes twice as thick?
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The net movement of particles from a region of higher concentration to a region of lower concentration, needing no energy from cells.
A tiny air sac in the lungs where gas exchange takes place; plural alveoli.
The narrowest type of blood vessel, with a wall one cell thick.
The difference in concentration between two regions, which drives diffusion.
The protein in red blood cells that binds oxygen, forming oxyhaemoglobin.
The measure scientists use for the concentration of a gas, for example in alveolar air or in blood.
A model stating that the rate of diffusion is proportional to surface area times concentration difference, divided by the thickness of the barrier.
In the lungs, oxygen diffuses from the air in the alveoli, across two thin layers of cells, into the blood and into red blood cells, because the blood arriving at the lungs has less oxygen than the air; in the body's tissues the gradient is reversed and oxygen diffuses out to the cells that use it.
This lesson works through the best-known example of diffusion in the body step by step. It follows an oxygen molecule from the alveoli into a red blood cell, explains why it moves (the concentration gradient) and how breathing, blood flow and haemoglobin keep that gradient steep, and then follows the oxygen out of the blood into a working muscle. It ends with the factors that control the rate of diffusion, including a simple worked calculation of how lung disease and altitude slow oxygen uptake.
Diffusion is the net movement of particles from a region of higher concentration to a region of lower concentration. It needs no energy from the cell. Gas exchange in the lungs is the clearest example of diffusion in the human body, so it is worth following one oxygen molecule on its journey.
Scientists measure the concentration of a gas as its partial pressure. In the alveoli, the partial pressure of oxygen is about 100 mmHg; in the blood arriving at the lungs it is about 40 mmHg. Oxygen therefore diffuses from the air into the blood until the blood leaving the lungs has almost the same oxygen level as the air in the alveoli.
If oxygen simply flowed in until both sides were equal, diffusion would stop. Three things prevent that:
In a working muscle, cells use oxygen in respiration all the time, so the oxygen concentration in and around them is low. When blood reaches the muscle's capillaries, the gradient is reversed: oxygen leaves haemoglobin, diffuses out of the red blood cell, across the capillary wall and into the muscle cells, where it is used in the mitochondria. Carbon dioxide made by respiration diffuses the opposite way, into the blood, and later out of the blood into the alveoli to be breathed out. The process is the same diffusion in each case; only the direction of the gradient changes.
A simple model of diffusion, known as Fick's law, says:
rate of diffusion ∝ (surface area × concentration difference) ÷ thickness of the barrier
Suppose oxygen normally diffuses into the blood at a rate R. If a lung disease doubles the thickness of the barrier, the rate becomes R ÷ 2, half the normal rate. If another disease destroys alveolar walls so that only 60% of the normal surface area remains, the rate falls to 0.6R. If both happened together, the rate would be 0.6 × 0.5 = 0.3, only 30% of normal. Altitude acts on the third factor: at high altitude the air holds less oxygen, so the concentration difference is smaller and oxygen diffuses into the blood more slowly, which is why climbers become breathless.