A 60° turn in an airplane doubles the g-force; how much g-force is experienced in a 15°, 30° and 45° turn?
Is it 0.5, 1 and 1.5g respectively?
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Sign up to join this communityA 60° turn in an airplane doubles the g-force; how much g-force is experienced in a 15°, 30° and 45° turn?
Is it 0.5, 1 and 1.5g respectively?
The formula for the load factor $n_z$ in a turn is
$$n_z = \frac{1}{cos\phi}$$
where $\phi$ is the bank angle. This makes the load factor in a 45° turn 1.414 or $\sqrt{2}$.
Since Michael correctly mentions the simplifications in his comment, let me expand the formula above. In case of a climbing turn, the load factor depends on the coordinate system used. If it is measured in airframe-fixed coordinates, the load factor will be split into a z-component ($n_z$, pointing down) and an x-component ($n_x$, pointing fore- or backward, depending on the aircraft's pitch attitude $\Theta$; nose-up is positive): $$n_x = -\frac{sin\Theta}{cos\phi}$$ $$n_z = \frac{cos\Theta}{cos\phi}$$
For an uncoordinated turn the value needs to be modified further with the relationship between bank angle change for a given sideslip angle, which is aircraft-specific.
The G forces (also known as the load factor) experienced by an aircraft and its occupants do not scale linearly with the bank angle of the aircraft.
Assuming constant vertical speed, coordinated flight (unchanging rate of climb or descent, ball centered), the load factor at a bank of 0° is 1.00. As the bank angle increases, this grows – slowly at first, then faster. At 15° the load factor is about 1.03; at 30°, about 1.15; at 45°, about 1.41. Increasing bank angle further, at 60° it's 2.00; at 75°, about 3.86.
In general, assuming level and coordinated flight, the load factor at a given bank angle $\theta$ is calculated as $$ n = \frac{1}{\cos{\theta}} $$
For example, for a bank angle $\theta = 45°$, we have $$ n = \frac{1}{\cos{45°}} \approx 1.41$$ and sure enough, the load factor for a level, 45° bank is just that.