When the star momentarily moves vertically
When the angle at the star of the spherical triangle is 90°
When the star's declination is greater than the observer's latitude
All the above
D. All the above
1 cm
2 cm
3 cm
4 cm
S - 90°
S - 180°
S - 270°
S - 360°
Elevation of the elevated pole
Declination of the observer's zenith
Angular distance along the observer's meridian between equator and the observer
All the above
B = bH/f
B =f/bH
B = b/fH
B = H/bf
58 mm
60 mm
62 mm
64 mm
The length of the air base is increased
The scale of the model is altered
y-parallax is not affected
All the above
Is the period of time taken by the earth in making a complete rotation with reference to stars
Is slightly shorter than an ordinary solar day
Is divided into the conventional hours, minutes and seconds
All the above
Always follow some definite mathematical law
Can be removed by applying corrections to the observed values
Are also known as cumulative errors
All the above
f tan θ
f sin θ
f cot θ
f cos θ
sin H = tan φ . cot δ
cos H = tan φ . cot δ
tan H = tan φ . cot δ
None of these
sin λ
cos λ
tan λ
cot λ
In truly vertical photographs without relief angles are true at the plumb point
In tilted photographs without relief, angles are true at the iso-centre
In tilled photographs with relief, angles are true at the principal point
None of these
North end of the polar axis is known as North Pole
South end of the polar axis is known as South Pole
Point where polar axis when produced northward intersects the celestial sphere, is known as north celestial pole
All the above
The measured stereoscopic base of photographs is obtained by dividing the air base in metres by the mean scale of the photograph
The difference between the absolute parallax of two points depends upon the difference in their elevations
The line joining the principal point of a photograph and the transferred principal point of the adjoining photograph, is called stereoscopic base
All the above
Refraction correction is zero when the celestial body is in the zenith
Refraction correction is 33' when the celestial body is on the horizon
Refraction correction of celestial bodies depends upon their altitudes
All the above
80°
70°
60°
50°
First point of Aeries
First point of Libra
Vernal Equinox
Both (b) and (d) of the above
Geodetic triangulation of greatest possible sides and accuracy is carried out
Primary triangles are broken down into secondary triangles of somewhat lesser accuracy
Secondary triangles are further broken into third and fourth order triangles, the points of which are used for detail surveys
All the above
Every angle is less than two right angles
Sum of the three angles is equal to two right angles
Sum of the three angles less than six right angles and greater than two right angles
Sum of any two sides is greater than the third
Zenith
Celestial point
Nadir
Pole
Plane surveying
Geodetic surveying
Star observations
Planet observations
High oblique
Low oblique
Vertical
None of these
North pole
Pole star
Celestial pole
All the above
At culmination
At elongation
Neither at culmination nor at elongation
Either at culmination or at elongation
θ = z + δ
θ = δ - z
θ = 180° - (z + δ)
θ = (z + δ) - 180°
10°
20°
30°
40°
Ursa Minor's remains always north of pole star
Polar star remains always north of Polaris
Polaris remains always north of Ursa Minor's
Ursa Minor's pole star and Polaris are the names of the same star
Declination
Altitude
Zenith distance
Co-latitude
Mean sun
First point of Aries
First point of Libra
The polar star
1 m
2 m
4 m
8 m