Translated Labs

YOU SAID:

In the Case of no vertical motion as shown in the right figure, the maximum value (3)(248.39) appeared on the non-linear side of the foundation rotational displacement due to the effect of parametric excitation as in the case of vertical motion , It is about 250 times greater than 3 and 10% of the secondary gradient of plastic.

INTO JAPANESE

右図のように上下動がない場合、上下動の場合と同様に、パラメトリック励振の影響により、最大値(3)(248.39)が基礎回転変位の非線形側に現れました。プラスチックの二次勾配の3および10%の約250倍です。

BACK INTO ENGLISH

As shown in the figure on the right, when there is no vertical movement, the maximum value (3) (248.39) appears on the nonlinear side of the basic rotational displacement due to the effect of parametric excitation, as in the case of vertical movement. It is about 250 times 3 and 10% of the secondary gradient of plastic.

INTO JAPANESE

右の図に示すように、垂直方向の動きがない場合、垂直方向の動きの場合のように、パラメトリック励起の効果により、最大値(3)(248.39)が基本回転変位の非線形側に現れます。 。これは、プラスチックの二次勾配の約250倍3および10%です。

BACK INTO ENGLISH

As shown in the figure on the right, when there is no vertical motion, as in the case of vertical motion, the maximum value (3) (248.39) appears on the nonlinear side of the fundamental rotational displacement due to the effect of parametric excitation. . . This is about 250 times 3 and 10% of the secondary gradient of plastic.

INTO JAPANESE

右の図に示すように、垂直運動の場合のように垂直運動がない場合、最大値(3)(248.39)は、パラメトリック励起の影響により基本回転変位の非線形側に現れます。 。 。 。これは、プラスチックの二次勾配の約250倍3と10%です。

BACK INTO ENGLISH

As shown in the figure to the right, when there is no vertical motion, as in the case of vertical motion, the maximum (3) (248.39) appears on the nonlinear side of the fundamental rotational displacement due to the effect of parametric excitation. . . . This is about 250 times 3 and 10% of the secondary gradient of plastic.

INTO JAPANESE

右の図に示すように、垂直運動の場合のように垂直運動がない場合、最大(3)(248.39)がパラメトリック励起の影響により基本回転変位の非線形側に現れます。 。 。 。これは、プラスチックの二次勾配の約250倍3と10%です。

BACK INTO ENGLISH

As shown in the figure to the right, when there is no vertical motion, as in the case of vertical motion, a maximum (3) (248.39) appears on the nonlinear side of the fundamental rotational displacement due to the effect of parametric excitation. . . . This is about 250 times 3 and 10% of the secondary gradient of plastic.

INTO JAPANESE

右の図に示すように、垂直運動の場合のように垂直運動がない場合、パラメトリック励起の効果により、基本回転変位の非線形側に最大(3)(248.39)が現れます。 。 。 。これは、プラスチックの二次勾配の約250倍3と10%です。

BACK INTO ENGLISH

As shown in the figure on the right, when there is no vertical motion, as in the case of vertical motion, a maximum (3) (248.39) appears on the nonlinear side of the fundamental rotational displacement due to the effect of parametric excitation. . . . This is about 250 times 3 and 10% of the secondary gradient of plastic.

INTO JAPANESE

右の図に示すように、垂直運動の場合のように垂直運動がない場合、パラメトリック励起の影響により、基本回転変位の非線形側に最大(3)(248.39)が現れます。 。 。 。これは、プラスチックの二次勾配の約250倍3と10%です。

BACK INTO ENGLISH

As shown in the figure on the right, when there is no vertical motion, as in the case of vertical motion, a maximum (3) (248.39) appears on the nonlinear side of the fundamental rotational displacement due to the effect of parametric excitation. . . . This is about 250 times 3 and 10% of the secondary gradient of plastic.

Equilibrium found!

You've done this before, haven't you.

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