Mathematics - Statics
Exam Duration: 45 Mins Total Questions : 30
The resultant of two forces P and Q is R. If Q is doubled,then R is doubled. If direction of Q is reversed, R is doubled again, then \({ P }^{ 2 }:{ Q }^{ 2 }:{ R }^{ 2 }\)is:
- (a)
2:3:2
- (b)
1:2:3
- (c)
2:3:1
- (d)
3:1:1
If the resultant of two forces of magnitudes P and 2P is perpendicular to P, then the angle between the forces, is
- (a)
\(\frac { 2\Pi }{ 3 } \)
- (b)
\(\frac { 3\Pi }{ 4 } \)
- (c)
\(\frac { 4\Pi }{ 5 } \)
- (d)
\(\frac { 5\Pi }{ 6 } \)
The resultant of two forces P and Q acting an angle \(\alpha \) is equal to \((2m+1)\sqrt { { P }^{ 2 }+{ Q }^{ 2 } } \) and when these forces act at an angle \(({ 90 }^{ \circ }-\alpha )\), the result is \((2m+1)\sqrt { { P }^{ 2 }+{ Q }^{ 2 } } \). then,\(\tan { \alpha } \) equals
- (a)
\(\frac { m+1 } {m-1 }\)
- (b)
\(\frac { m } {m+1 }\)
- (c)
\(\frac { m-1 } {m+1 }\)
- (d)
\(\frac { m } {m-1 }\)
Two forces P and Q acting at a point are such that if one of these is reversed, the direction of the resultant is turned through a right angle, then
- (a)
P=2Q
- (b)
2P=Q
- (c)
2P=3Q
- (d)
P=Q
If the resultant of two equal forces inclined at an angle \(2{\theta}\) is twice as grest as when these are inclined at an angle \(2\Phi \),then
- (a)
\(2\cos { \theta } =\cos { \phi } \)
- (b)
\(\cos { \theta } =2\cos { \phi } \)
- (c)
\(\theta =\Pi \)
- (d)
None of these
The greatest resultant of two forces is P and least resultant is Q. when these forces act an angle \(\theta\), then the resultant ,is
- (a)
\(\sqrt { ({ P }^{ 2 }{ sin }^{ 2 }(\frac { \theta }{ 2 } )+{ Q }^{ 2 }{ cos }^{ 2 }(\frac { \theta }{ 2 } ) } \)
- (b)
\(\sqrt { ({ P }^{ 2 }{ +Q }^{ 2 } } \)
- (c)
\(\sqrt { { P }^{ 2\quad }{ cos }^{ 2 }(\frac { \theta }{ 2 } )+{ Q }^{ 2 }{ sin }^{ 2 }(\frac { \theta }{ 2 } ) } \)
- (d)
None of these
The resultant of two forces P and Q is \(\sqrt { 3 }\)Q and makes an angle \({ 30 }^{ \circ }\)with the direction of P. then
- (a)
P=Q or P=2Q
- (b)
P=Q or Q=2P
- (c)
P=2Q or Q=3P
- (d)
P=Q or P=4Q
The resultant R of two forces P and Q act at right angles to P. Then the angle between these forces, is
- (a)
\({ cos }^{ -1 }(\frac { P }{ Q } )\)
- (b)
\({ cos }^{ -1 }(-\frac { P }{ Q } )\)
- (c)
\({ sin }^{ -1 }(\frac { P }{ Q } )\)
- (d)
\({ sin }^{ -1 }(-\frac { P }{ Q } )\)
The resultant of two equals forces acting on a particle is equal to three times the product of these forces. then angle between these forces is:
- (a)
\({ 30 }^{ \circ }\)
- (b)
\({ 45 }^{ \circ }\)
- (c)
\({ 60 }^{ \circ }\)
- (d)
\({ 90 }^{ \circ }\)
A weight of 26 N is suspended by two light inelastic strings of length 5m and 12m from two points at the same level 13m apart. Then tensions in the strings are
- (a)
24N,10N
- (b)
28N,12N
- (c)
24N,16N
- (d)
None of these
Three forces of magnitude 8N,5N and 4N acting at a point are in equilibrium, then the angle between smaller forces is:
- (a)
\({ cos }^{ -1 }(\frac { 21 }{ 40 } )\)
- (b)
\({ cos }^{ -1 }(\frac { 23 }{ 40 } )\)
- (c)
\({ cos }^{ -1 }(\frac { 20 }{ 39 } )\)
- (d)
\({ cos }^{ -1 }(\frac { 23 }{ 39 } )\)
The line of action of the resultant of two forces P and Q divides the angle between them in the ration 1:2. then the magnitude of their resultant is:
- (a)
\(\frac { { Q }^{ 2 }-{ P }^{ 2 } }{ Q } \)
- (b)
\(\frac { { P }^{ 2 }-{ Q }^{ 2 } }{ P } \)
- (c)
\(\frac { { P }^{ 2 }-{ Q }^{ 2 } }{ Q } \)
- (d)
\(\frac { { P }^{ 2 }+{ Q }^{ 2 } }{ { P }^{ 2 }-{ Q }^{ 2 } } \)
Two men carry a straight uniform bar 16m long weighing 80 kg.One man supports the bar at a distance of 2m from one end and the other at a distance of 3m from the other end.Then the weight on each man, is
- (a)
\(43\frac { 7 } { 11 }kg,36\frac { 4 } { 11 }kg\)
- (b)
\(36\frac { 7 } { 11 }kg,43\frac { 4 } { 11 }kg\)
- (c)
44kg,36kg
- (d)
None of these
Three like parallel forcesP,Q and R act at the vertices of a triangle ABC.If the line of action of the resultant passes through the orthocentre
- (a)
\(\frac { P } {a }=\frac { Q } {b }=\frac { R } {c }\)
- (b)
\(\frac { P } {sin 2A }=\frac { Q } {sin2b }=\frac { R } {sin2c }\)
- (c)
\(\frac { P } {tanA }=\frac { Q } {tanB }=\frac { R } {tanC }\)
- (d)
None of these
Two like parallel forces 5N and 15N, act on a light rod at two points A and B respectively, 6m apart.The magnitude of resultant and the distance of its point of action from the point A, are respectively
- (a)
10N;4.5m
- (b)
20N;4.5m
- (c)
20N;1.5m
- (d)
10N;1.5m
Three like forces P,Q,R act at vertices of a triangle ABC.If their resultant passes through the circumcentre of \(\Delta ABC\),then
- (a)
\(\frac { P }{ a } =\frac { Q }{ b } =\frac { R }{ c } \)
- (b)
\(\frac { P }{ sin2A } =\frac { Q }{ sin2B } =\frac { R }{ sin2C } \)
- (c)
\(\frac { P }{ tan A } =\frac { Q }{ tan B } =\frac { R }{ tan C } \)
- (d)
None of these
A man can exert a force of 100N and pulls on a rope fastened to the top of a post, the length of the rope beiong twice the length of the post.The horizontal force applied to the middle of the post that will keep it fromfailing, is
- (a)
100N
- (b)
200N
- (c)
\(100\sqrt { 3}\)N
- (d)
200N
Three forces P,Q,R act along the sides BC,CA and AB of the triangle ABC.If their resultant passes through their centroid, then
- (a)
\(\frac { P }{ a } =\frac { Q }{ b } =\frac { R }{ c } =0\)
- (b)
P sec A+Q sec B+R sec C=0
- (c)
P cot A+Q cot B+R cot C=0
- (d)
P tan A+Q tan B+R tan C=0
Forces of magnitudes 1N,2N,3N,4N,5N and 6N act along OA,OB,OC,OD,OE and OF respectively,where ABCDEF is a regular hexagon with O as centre.Then the angle which the resultant makes with OC, is
- (a)
\({ 30 }^{ \circ }\)
- (b)
\({ 45 }^{ \circ }\)
- (c)
\({ 60 }^{ \circ }\)
- (d)
\({ 120 }^{ \circ }\)
Forces P and Q whose resultant is R act at point O. A transveral is drawn meeting lines of action of these forces at L,M and N respectively.then,\(\frac { p} {OL}+\frac { Q} { OM }\)equals
- (a)
\(\frac { R } { PL+OM}\)
- (b)
\(\frac { R } { ON }\)
- (c)
\(\frac { R } { OL-OM }\)
- (d)
None of these
If the forces are represented by the sides of a triangle taken in order, then these are equivalent to
- (a)
a couple
- (b)
a force of non-zero magnitude
- (c)
a force of zero magnitude
- (d)
a force and a couple
Forces,each of magnitude P, act in the directions parallel to the sides BC,CA and Ab of the triangle ABC. Then magnitude of the resultant, is
- (a)
\((\sqrt { 1-2\cos { A } -2\cos { B } -2\cos { C } } )P\)
- (b)
\((\sqrt { 3-2\cos { A } -2\cos { B } -2\cos { C } } )P\)
- (c)
\((\sqrt { 3-\cos { A } -\cos { B } -\cos { C } } )P\)
- (d)
None of these
Two forces acting at the point A (-3,0) and B(3,0) form a couple of moment 30 units.If AB is the arm of the couple then magnitude of each of these forces, is
- (a)
5 units
- (b)
6 units
- (c)
8 units
- (d)
10 units
Two forces P and Q acting parallel to the length and base of inclined plane respectively would each of them singly support weight W on the plane;then \(\frac { 1 }{ { P }^{ 2 } } -\frac { 1 }{ { Q }^{ 2 } } \)equals
- (a)
\(\frac { 2 }{ { W }^{ 2 } } \)
- (b)
\(\frac { 4 }{ { W }^{ 2 } } \)
- (c)
\(\frac { 1 }{ { W }^{ 2 } } \)
- (d)
None of these
A horizontal force F is applied to a small object P of mass m on a smooth plane inclined at an angle \(\theta\) to the horizontal. If F is just enough to keep theobject in equilibrium, then magnitude of F is
- (a)
\(mg\quad { cos }^{ 2 }\theta \)
- (b)
\(mg\quad { sin }^{ 2 }\theta \)
- (c)
\(mg { cos }\theta \)
- (d)
\(mg\quad { tan }\theta\)
A practicle is acted upon by three forces P,Q and R.It cannot be in equilibrium, if P:Q:R, is
- (a)
1:3:5
- (b)
3:5:7
- (c)
5:7:9
- (d)
7:9:11
A couple is of moment \(\overrightarrow { G } \) and the force forming the couple is \(\overrightarrow { P } \).If \(\overrightarrow { P } \) is turned a right angle the moment of the couple thus formed is \(\overrightarrow { H }\). If instead, the forces \(\overrightarrow { P } \). are turned through an angle \(\alpha\), then the moment of the couple is:
- (a)
\(\overrightarrow { H } \cos { \alpha } +\overrightarrow { G } \sin { \alpha } \)
- (b)
\(\overrightarrow { G } \cos { \alpha } +\overrightarrow { H } \sin { \alpha } \)
- (c)
\(\overrightarrow { H } \sin { \alpha } -\overrightarrow { G } \cos { \alpha } \)
- (d)
\(\overrightarrow { G } \sin { \alpha } +\overrightarrow { H } \cos { \alpha } \)