12th Grade > Physics
CALCULUS MCQs
Total Questions : 29
| Page 3 of 3 pages
Answer: Option A. -> −cos 8x8+x22+c
:
A
∫(sin(8x)+x)dx=∫sin(8x)dx+∫(x)dx
8x = t
8dx = dt
dx = dt8
⇒∫sintdt8+x22+c1 (∵∫xndx=xn+1n+1)+c
⇒−cost8+co+x22+c (∵∫sintdt=−cost)
−cos8x8+x22+c (c=c0+c1)
:
A
∫(sin(8x)+x)dx=∫sin(8x)dx+∫(x)dx
8x = t
8dx = dt
dx = dt8
⇒∫sintdt8+x22+c1 (∵∫xndx=xn+1n+1)+c
⇒−cost8+co+x22+c (∵∫sintdt=−cost)
−cos8x8+x22+c (c=c0+c1)
Answer: Option A. -> 3b4at
:
A
This is called implicit differentiation or indirect differentiation. Here both the terms given are differentiatedindependently w.r.t a third variable and then combined together. Differentiating x and y w.r.t 't'
dxdt=4at3,dydt=3bt2
Diving dydtbydxdt,dydx=dydt×dtdx=3bt24at3=3b4at
:
A
This is called implicit differentiation or indirect differentiation. Here both the terms given are differentiatedindependently w.r.t a third variable and then combined together. Differentiating x and y w.r.t 't'
dxdt=4at3,dydt=3bt2
Diving dydtbydxdt,dydx=dydt×dtdx=3bt24at3=3b4at
Answer: Option C. -> x22−lnx−1x+c
:
C
∫ydx=∫xdx−∫1xdx+∫1x2dx
= x22−lnx−x−2+1−2+1+c
= x22−lnx−1x+c
:
C
∫ydx=∫xdx−∫1xdx+∫1x2dx
= x22−lnx−x−2+1−2+1+c
= x22−lnx−1x+c
Answer: Option B. -> −12x32
:
B
Differentiating both sides w.r.t. x,
dydx=d[(x)−12]dx=−12x−32=−12x32
:
B
Differentiating both sides w.r.t. x,
dydx=d[(x)−12]dx=−12x−32=−12x32
Answer: Option B. -> π200
:
B
y= sinx
dydx is instantaneous rate of change = cosx
Question is asking change in y i.e. △y
given △x i.e., π3toπ3+π100
⇒△x=π100
Since rate is asked to be assumed approximately the same as instantaneous rate so
dydx=△y△x
dydxatx=π3=cosπ3=12
12=△yπ100,△y=π200
:
B
y= sinx
dydx is instantaneous rate of change = cosx
Question is asking change in y i.e. △y
given △x i.e., π3toπ3+π100
⇒△x=π100
Since rate is asked to be assumed approximately the same as instantaneous rate so
dydx=△y△x
dydxatx=π3=cosπ3=12
12=△yπ100,△y=π200
Answer: Option C. -> 2cosx+4secx tanx+4cosec2x
:
C
y= 2sinx + 4secx - 4cotx
dydx=d(2sinx+4secx−4cotx)dx
=d(2sinx)dx+d(4secx)dx+d(−4cotx)dx
=2dsinxdx+4d(secx)dx−4d(cotx)dx
=2cosx+4secxtanx−4(−cosec2x)
=(sincedsinxdx=cosx;dsecxdx=secxtanx;dcotxdx=−cosec2x)
dydx=2cosx+4secxtanx+4cosec2x
:
C
y= 2sinx + 4secx - 4cotx
dydx=d(2sinx+4secx−4cotx)dx
=d(2sinx)dx+d(4secx)dx+d(−4cotx)dx
=2dsinxdx+4d(secx)dx−4d(cotx)dx
=2cosx+4secxtanx−4(−cosec2x)
=(sincedsinxdx=cosx;dsecxdx=secxtanx;dcotxdx=−cosec2x)
dydx=2cosx+4secxtanx+4cosec2x
Answer: Option B. -> x√x2+1
:
B
y=√x2+1
x2+1=u....(1)
⇒dudx=2x....(2)
⇒y=√u
Now, dydx=dydu×dudx
=12√u×dudx
=12√x2+1×2x From (1) & (2)
dydx=x√x2+1
:
B
y=√x2+1
x2+1=u....(1)
⇒dudx=2x....(2)
⇒y=√u
Now, dydx=dydu×dudx
=12√u×dudx
=12√x2+1×2x From (1) & (2)
dydx=x√x2+1
Answer: Option B. -> aL+bL22
:
B
We cannot calculate the mass of the rod by simply multiplying linear mass density '′λ′ will the length of the rod as ′λ′ is not constant.
Hence we have to divide entire rod length into a number of elements and add the mass of all elements.
M=dm1+dm2+dm3+.......
This step can be written in terms of integration.
M=∫dm
If we take an element dx on the rod at a distance x from the left end of the rod.
Mass of this element dm=λ.dx
dm=(a+bx)dx
Hence total mass M=∫dm⇒M=L∫0(a+bx)dx
M=L∫0adx+L∫0bxdx=aL∫0dx+bL∫0xdx=a[x]L0+b[x22]L0⇒M=aL+bL22
:
B
We cannot calculate the mass of the rod by simply multiplying linear mass density '′λ′ will the length of the rod as ′λ′ is not constant.
Hence we have to divide entire rod length into a number of elements and add the mass of all elements.
M=dm1+dm2+dm3+.......
This step can be written in terms of integration.
M=∫dm
If we take an element dx on the rod at a distance x from the left end of the rod.
Mass of this element dm=λ.dx
dm=(a+bx)dx
Hence total mass M=∫dm⇒M=L∫0(a+bx)dx
M=L∫0adx+L∫0bxdx=aL∫0dx+bL∫0xdx=a[x]L0+b[x22]L0⇒M=aL+bL22
Answer: Option D. -> xcosx−sinxx2
:
D
y=sinxx
dydx=xddx(sinx)−sinx(dxdx)x2
=xcosx−sinxx2
:
D
y=sinxx
dydx=xddx(sinx)−sinx(dxdx)x2
=xcosx−sinxx2