| CPC F02C 9/24 (2013.01) [F01D 19/00 (2013.01); F02C 9/18 (2013.01); F02C 7/268 (2013.01); F02C 7/36 (2013.01)] | 20 Claims |

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1. A method of operating a gas turbine engine on an aircraft, the gas turbine engine comprising:
an engine core comprising a turbine, a combustor, a compressor, and a core shaft connecting the turbine to the compressor;
a fan located upstream of the engine core, the fan comprising a plurality of fan blades;
a nacelle surrounding the engine core and defining a bypass duct and a bypass exhaust nozzle; and
a gearbox that receives an input from the core shaft and outputs drive to the fan so as to drive the fan at a lower rotational speed than the core shaft, wherein the method comprises operating the gas turbine engine to provide propulsion such that a jet velocity ratio, RJ, of a first jet velocity exiting from the bypass exhaust nozzle to a second jet velocity exiting from an exhaust nozzle of the engine core is defined as:
![]() where VB is a fully expanded first jet velocity, CB is a thrust coefficient of the bypass exhaust nozzle, VC is a fully expanded second jet velocity, CC is a thrust coefficient of the engine core exhaust nozzle, ηLPT is an isentropic efficiency of a lowest pressure turbine of the engine core and ηF is an isentropic efficiency of a fan tip;
the jet velocity ratio, RJ, is between around 0.75 and 1.3 at maximum take-off conditions;
each fan blade has a radial span extending from a hub to a tip, and a ratio of a radius of each fan blade at its hub to a radius of each fan blade at its tip is in a rang of 0.25 to 0.4;
a bypass ratio, defined as a ratio of a mass flow rate of a flow through the bypass duct to a mass flow rate of a flow through the core at cruise conditions, is in a range of 10 to 17;
a fan tip loading defined as dH/Utip2 is between 0.28 and 0.38 at cruise conditions, where dH is an enthalpy rise across the fan and Ud is a translational velocity of the leading edge of a fan tip; and a specific thrust, defined as a net thrust of the engine divided by a total mass flow through the engine, is between 80 Nkg-1s and 110 N kg−1s at the cruise conditions.
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