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JGP Ostrava 2022: Mao Shimada Quad toe

Updated: 3 days ago

The Czech figure skating federation held the second Junior Grand Prix this season, which was exciting to watch. I had the chance to be there to record a few triple axle and quad toe loops (4T). Let’s talk about Mao Shimada from Japan. The first analysis highlights the toe-pick leg, how Mao moves her leg, and makes contact with the ice. It was shot during the official training.

Mao Shimada is a Japanese figure skater with a decorated career. She is also the 21st and second Japanese woman to land a triple Axel jump and quadruple toe-loop in competition.


Advanced analysis with stromotion effect of quad toe of Mao SHIMADA during the training at Junior Grand Prix Ostrava 2022
Advanced analysis with stromotion effect of quad toe of Mao SHIMADA during the training at Junior Grand Prix Ostrava 2022

The first analysis highlights the toe-pick leg, how Mao moves her leg, and makes contact with the ice. It was shot during the official training. The launch angle combines the skater’s vertical and horizontal velocity at the take-off. Having ice contact with the entire blade influences the launch angle a lot. To make it short ( I planned to explain the importance of the launch angle in another blog), the skater is getting off the ice to fly as long as possible.


 

Detail of quad toe of MaoSHIMADA during the training at Junior Grand Prix Ostrava 2022

Detail  toe pick of quad toe of MaoSHIMADA during the training at Junior Grand Prix Ostrava 2022

During the 6-minute warm-up, Mao succeeded in one quad-toe loop, but unfortunately, there was no video. From the Free Skating (FS) ISU broadcast, we can get this view to understand better why Shimada moves her free leg like this. In every jump, preparation is the most important; here, it’s the 3-turn.


Detail of quad toe of MaoSHIMADA during the warm-up of the Free Skating  at Junior Grand Prix Ostrava 2022

During the two feet part of the preparation, we can see that her body weight is not correctly on her right axis. The next move is the foot change, meaning she should anticipate this and transfer her weight to the right leg. It explains why she is changing her edge (inside->outside).


Detail of quad toe of Mao SHIMADA during the warm-up of the Free Skating  at Junior Grand Prix Ostrava 2022

For a triple toe, it’s not so important; it’s recommended to do a quick change of edge but for a quad. Each aspect of the preparation must be optimized.

Detail of quad toe of Mao SHIMADA during the warm-up of the Free Skating  at Junior Grand Prix Ostrava 2022

Her inside backward edge is making her unbalanced. The main consequence is opening the left hip to tap the ice too much. On this attempt, her Center Of Mass (C.O.M., noted with the blue arrow below) is almost aligned with her toe picks. However, the vertical velocity direction is ineffective (red arrow).


Detail of quad toe of Mao SHIMADA during the warm-up of the Free Skating  at Junior Grand Prix Ostrava 2022

This stromotion is done from the video I filmed from the audience, a profile view to add more value to the ISU video.


Advanced analysis with stromotion effect of quad toe of Mao SHIMADA during the Free Skating at Junior Grand Prix Ostrava 2022

The preparation is long. Mao takes from the moment she is backward to tap the ice 1,478 seconds (On average, 0,768 seconds). The approaching speed with a start backward and then a turn generates a compelling angular momentum. Mao doesn’t use this effect so much.

Detail of quad toe of Mao SHIMADA during the Free Skating at Junior Grand Prix Ostrava 2022

In this picture, we can see that she holds a lot of her head.


Detail of quad toe of Mao SHIMADA during the Free Skating at Junior Grand Prix Ostrava 2022

The result is a landing called < (Under-rotated). That’s why she fell.

This jump had a more extended flight time (Ft) than was recorded during the training. 0.638s in the air instead of 0.604s. The snap's angular velocity (when the skater takes off to the final air position) is almost the same in both studied jumps ( around 28 radians per second).


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