Eba Station
Eba Station is a Hiroden terminal station on the Hiroden Eba Line located in Eba-nishi, Naka-ku, Hiroshima. A streetcar and bus depot, is located behind the station. The station is operated by the Hiroshima Electric Railway.
Eba 江波 | |
|---|---|
 | |
| Location | Eba-nishi 1-chome, Naka-ku, Hiroshima Japan |
| Coordinates | 34.3724°N 132.4360°E |
| Operated by | Hiroshima Electric Railway |
| Line(s) |
|
| Platforms | 2 side platforms |
| Other information | |
| Station code | E6 |
| History | |
| Opened | June 20, 1944 |
Routes
There are three routes that serve Eba Station:
- 6 Hiroshima Station - Eba Route
- 8 Yokogawa Station - Eba Route
- 9 Hakushima - Eba Route
Station layout
The station consists of two side platforms serving two tracks. There is a large shelter located on the outbound platform.
Adjacent stations
| « | Service | » | ||
|---|---|---|---|---|
| Hiroden Eba Line | ||||
| Funairi-minami-machi | Route 6 | Terminus | ||
| Funairi-minami-machi | Route 8 | Terminus | ||
| Funairi-minami-machi | Route 9 | Terminus | ||
Bus connections
- Hiroden Bus Route #6 at Hiroden Eba Office bus stop
Surrounding area
- Hiroshima City Ebayama Museum of Meteorology
- Mitsubishi Heavy Industries Hiroshima Machinery Works
- Hiroden Eba-shako - (streetcar and bus shed)
- Hiroden Eba Office
- Hiroshima City Eba Junior High School
- Hiroshima Municipal Eba Elementary School
- Eba Shrine
History
- Opened on June 20, 1944.
- Renamed to "Eba-guchi" on November 1, 1947.
- Moved on January 7, 1954 when the train and bus shed was built.
- Renamed to "Eba" in 1963.
gollark: This is actually somehow really accurate.
gollark: True engineers approximate the pendulum time period formula $T=2\pi \sqrt{\frac{l}{g}}$ as $T=2\sqrt{l}$.
gollark: So basically just "optics but we are HIGHLY engineer-like and use the small angle approximation".
gollark: According to Wikipedia, which I just checked, which makes me an expert,> Gaussian optics is a technique in geometrical optics that describes the behaviour of light rays in optical systems by using the paraxial approximation, in which only rays which make small angles with the optical axis of the system are considered. In this approximation, trigonometric functions can be expressed as linear functions of the angles. Gaussian optics applies to systems in which all the optical surfaces are either flat or are portions of a sphere. In this case, simple explicit formulae can be given for parameters of an imaging system such as focal length, magnification and brightness, in terms of the geometrical shapes and material properties of the constituent elements.
gollark: Fearsome.
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