· The vertical sound speed is derived from the Munk canonical profile, and propagation is...

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Transcript of  · The vertical sound speed is derived from the Munk canonical profile, and propagation is...

Page 1:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 2:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 3:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 4:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 5:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 6:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 7:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 8:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 9:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 10:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 11:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 12:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 13:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 14:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 15:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 16:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 17:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above
Page 18:  · The vertical sound speed is derived from the Munk canonical profile, and propagation is calculated using a wide angle parabolic equation (PE) code. The narrow beam source is above

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