M. Kemal Ozgoren - Kinematics of General Spatial Mechanical Systems
Здесь есть возможность читать онлайн «M. Kemal Ozgoren - Kinematics of General Spatial Mechanical Systems» — ознакомительный отрывок электронной книги совершенно бесплатно, а после прочтения отрывка купить полную версию. В некоторых случаях можно слушать аудио, скачать через торрент в формате fb2 и присутствует краткое содержание. Жанр: unrecognised, на английском языке. Описание произведения, (предисловие) а так же отзывы посетителей доступны на портале библиотеки ЛибКат.
- Название:Kinematics of General Spatial Mechanical Systems
- Автор:
- Жанр:
- Год:неизвестен
- ISBN:нет данных
- Рейтинг книги:4 / 5. Голосов: 1
-
Избранное:Добавить в избранное
- Отзывы:
-
Ваша оценка:
Kinematics of General Spatial Mechanical Systems: краткое содержание, описание и аннотация
Предлагаем к чтению аннотацию, описание, краткое содержание или предисловие (зависит от того, что написал сам автор книги «Kinematics of General Spatial Mechanical Systems»). Если вы не нашли необходимую информацию о книге — напишите в комментариях, мы постараемся отыскать её.
This all-time beneficial book:
Provides an easy-to-use systematic formulation method that is applicable to all sorts of spatial machanisms and manipulators Introduces a symbolic manipulation method, which is effective and straightforward to use, so that kinematic relationships can be simplified by using all the special geometric features of the system Offers an accessible format that uses a systematic and easy-to-conceive notation which has proven successful Presents content written by an author who is a renowned expert in the field Includes an accompanying website Written for academicians, students, engineers, computer scientists and any other people working in the area of spatial mechanisms and manipulators,
provides a clear notation, formulation, and a logical approach to the topic and offers a fresh presentation of challenging material.

must not bear ( a ) because it is a vector that is specified without necessarily knowing anything about the observation frame
, whereas
must necessarily bear ( a ) because it is one of the basis vectors of
. In Eq. (1.38), on the other hand,
must necessarily bear ( a ) because it represents the appearance of
as observed in
, whereas
must not bear ( a ) because it is not tied up to any reference frame as explained above and expressed by Eq. (1.36).
and
, which are resolved as follows in a reference frame
:

and
can be expressed as



and
, which are the column matrix representations of
and
in
:

.
and
, which are expressed by Eqs. (1.40)and (1.41)as resolved in the reference frame
. Their cross product can be expressed as




