Dataset Viewer
audio
audioduration (s) 0.15
121
| text
stringlengths 1
131
| path
stringlengths 78
81
|
---|---|---|
us see that. So, if I write the equation of motion, I will
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vlQWM_PZNx4_26.wav
|
|
n 1 factorial, n 2 factorial, so what will I do for this thing? So, you tell me something
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vmb0mcCtqMM_397.wav
|
|
distinct network. So, if it is in to a 2 distinct networks you may use different switching
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vn7aT9-cYzQ_182.wav
|
|
take between the integral 0 and 1 x 3 x square d x, you get excepted value of x is 3 by 4,
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vnAWreeG2a8_82.wav
|
|
this equivalent to some resistance R prime here. No, some resist the same resistance R, but it turns ratio
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vnjxmqBeitg_210.wav
|
|
remain forever. So, we cannot say that, the rows will become identical in the sense
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vo2fX9thVQU_317.wav
|
|
plant, when the concentration or the pressure or the temperature changes, the corrective
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vo7LN-zMI2s_115.wav
|
|
gets cleared in the grounding resistor. The other ways of doing, people have also looked
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vos7G_mRxYc_94.wav
|
|
the region of k 1; it contains neither k 2 nor k 3 so, d two is 1 0 0. D 3 is shown as
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/votLpZSfkF8_291.wav
|
|
Basically, that is what I was saying. That method of characteristics being very well
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vp0OUpnxPGg_151.wav
|
|
So, the input to is one and the data format may change from one to another and the individual
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vp4fjie0ENA_34.wav
|
|
is not greater than equals 0 for all j for this two for j equals 1 and j equals 2 Z j
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vpPJYJwWkNU_250.wav
|
|
have some bubbles. Which side you measure? Whatever side you focus, that is not uniformly
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vpvb6JQWy44_209.wav
|
|
d z has to be equal to 0. So, this completes this example with these estimation theorems.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vq2oaeQbXmQ_181.wav
|
|
because even for a white noise process, when you take a specific realization and compute
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vqIxYJa0Dz4_12.wav
|
|
wherein you have an even function on sin theta, an even function of argument and theta goes
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vrE7lQ81xmo_367.wav
|
|
So, that was the whole idea of generating this particular turbulence model.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vrqDSqwMuH8_130.wav
|
|
to produce the gear tooth profile okay. So, in this case the tooth will be like this.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vsNAPRIKAVs_359.wav
|
|
that we have noticed here that except the point f 1 x is equal to k f naught at other
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vsQ6xvj7pnQ_8.wav
|
|
if i is equal to s it is aij if i is not equal to s so I am just calling this as a new matrix
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vsXNCnSPU9I_185.wav
|
|
talked about ab is equal to 0 or ab is nearly equal to 0 which means, it is not going to
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vsfQU4ofQ-Y_315.wav
|
|
Here, what is important is that I do not attach any value to the time that I am spending in
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vsn3nZcbpdY_190.wav
|
|
this rectangle that is on this x-axis is the same as this one.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vt1_7f5l3hI_297.wav
|
|
is various parameters. We can do lot more variations in the case of simulations base
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vtAT6ipxc0A_54.wav
|
|
alpha and summation of these three vectors namely O2A plus AB plus BC which is nothing
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vtY8Sn3wuRU_48.wav
|
|
much fleet we are talking about. If it 75% of the fleet, then the runway length required
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vtkbeigLTzQ_69.wav
|
|
E 0 z and since I am going to be using spherical symmetry let me write it as minus E 0 z
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vtvY1PZKLQM_392.wav
|
|
Now, let us take the quarter model and discretized that using four linear triangle elements four
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vtxM79BOcqs_212.wav
|
|
I am going to get it right here r, t, f so far playing top and right side of the box right. So,
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vu1VNKHfzqQ_223.wav
|
|
mode.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vu6eLFmrwaA_354.wav
|
|
is based on the deactivation timescales, as dictated by the corresponding decay constant. So, let
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vuIG4vKUDA0_302.wav
|
|
Substantively of naphthols: Why is it important to discuss so much about it?
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vvO8VCqiwNo_107.wav
|
|
and power.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vwOE1HVViQM_163.wav
|
|
that these three membered ring is possible.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vwq8UpQC1lw_188.wav
|
|
sand is subjected to either direct shear or triaxial shear. Dense sands undergo an expansion,
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vx6_ALfiTBI_384.wav
|
|
functions. Corresponding to the indeces i N p N p plus i are basis functions of order
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/vyLjdVjXgLo_313.wav
|
|
they pass to an aromatic; generally they pass to an aromatic transition state; that is very
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w0xxH28iZhY_50.wav
|
|
I say that I have a wave which is approaching form this side than what should be my progressive,
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w1GKZZbaVPE_165.wav
|
|
So h1 is injective and holomorphic therefore again by inverse mapping theorem h1 will give
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w3IgSabA_no_95.wav
|
|
slowly from laminar flow to fully turbulent flow and that is represented by this kind
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w3KbN3n7hSc_356.wav
|
|
is F y prime F y prime we put q E y E y prime. So, I substitute things in this particular
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w6w48G4Kfmk_425.wav
|
|
gave us a solution with two machines but it did not have any restriction on the cycle
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w7kKp5QC5_4_14.wav
|
|
evident clearly will tell us whether the person has learned about the brand and the brand
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w8f34-DZlm8_428.wav
|
|
concentrate on one wavelength here through the gap of D and see what the flow rate is.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w8g_0rcb2q0_137.wav
|
|
this.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/w9Gh1XFpLqc_532.wav
|
|
what is the opposite of attracter
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wAUwtSLkZ94_243.wav
|
|
grinding wheel like the Ceramic wheel Aluminum Oxide wheel or Silicon Carbide wheel So this
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wAX8I35xw1o_365.wav
|
|
of the line? You know you looking at this segment, of course this part and this part
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wCJKm1eMscg_86.wav
|
|
Let us take a memory reference operation and in our instruction said, we have put only
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wCm3f-rWF20_207.wav
|
|
still remains infinity. So, I have 0 to infinity eta to the power of half into d eta divided
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wELT9TPO1mA_163.wav
|
|
400 kilo volt. So, once there is AC dip this, because the firing will be same automatically
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wFWoNto9phg_58.wav
|
|
three okay. And another example we have was that if we
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wFujtazGFeE_42.wav
|
|
the standard practice in optimization literature. So, question arise is, is follows number 1
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wGFFxY1gxSU_13.wav
|
|
velocity was the major kinetic characterization of soluble enzyme which gives you information
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wIhVqHZjOIw_365.wav
|
|
probability of root n x bar minus 1 less than or equal to minus root n, that is equal to
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wKMhBo6zelc_117.wav
|
|
types of condition.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wKPmO8DTWdQ_40.wav
|
|
Now, was proposed by Einstein’s. So, you have Einstein’s theory of general relativity
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wKrzeisn5SU_420.wav
|
|
able to simplify the matters a lot from here. This is f 0 g 1 2 there will be 0 here so
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wLKfRNYYWf4_146.wav
|
|
say the kernel func ahh the parameters list right whatever is in the parenthesis and also
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wLZ7F8LDo1c_329.wav
|
|
have all the way direction is.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wLoRhkfWOp0_218.wav
|
|
whom I do not want to allowing in my shopping mall. And assume a system false, face system
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wM7owQ-GEks_293.wav
|
|
Other words, I said finger print for instance finger print recognition is there.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wMIK2_GUsJg_109.wav
|
|
both radially as well as in the circumferential direction. Again this 2 D equation can be
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wMe_UNem7B4_352.wav
|
|
or few multiples of it at the most maybe if it is 10 times the fundamental rate this could
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wMzPW2-80rM_175.wav
|
|
observation the second observation is you see ah if i replace ah e z by e z plus one
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wNueayo7w4s_143.wav
|
|
one can manually balance and then one have to measure this voltage and this voltage.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wOJz93c69nA_100.wav
|
|
can you make? You cannot make bigger. You cannot make more than 50 liters or 100 liters
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wOPOPN1s4Gk_370.wav
|
|
agents zero sum games as a search problem. They will learn how to apply the mini max
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wP3mDYnHx74_153.wav
|
|
microfluidic devices which are used in several biological and bio-technological applications.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wPLy8KNxso8_275.wav
|
|
percent, 15 percent, as the time passes there will be greater and greater percentage of
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wT120FJqX_g_224.wav
|
|
for every particle there is an associated waves so, let we write down a wave. We are
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wTcRbscozPI_256.wav
|
|
This pinion rotates in the clockwise direction, drives the rack to the left.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wzZdMZxKwF4_37.wav
|
|
Jacobian matrix you are going to get rank less than, you will not get rank uhh n minus
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/wzpEO3tZJAE_457.wav
|
|
this population variance of thispopulation. So, this ratio multiplied by the n minus 1so
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x-Gn-sxbIVU_319.wav
|
|
remain inside is cosine theta minus alpha plus cosine theta plus alpha . Further expansion
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x-WlcmsNkrE_46.wav
|
|
But you see this is what will happen in in practice and uhhh but the fact is even if
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x-_t7wW_4x0_101.wav
|
|
House describes charismatic leaders as those who have charismatic effects on the followers
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x-ycseyaPDE_292.wav
|
|
Now, another template that people use quite often are what are called nucleopore membranes,
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x-zC6VqPz3M_269.wav
|
|
it is that it is a critical session meaning that at this point that parallel thinks are
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x0fyA_4PP_U_255.wav
|
|
So, you will be getting the sine functions as the Eigen functions and sine and the Eigen
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x0tL8pp4ELg_170.wav
|
|
by four h cross square and xi square plus eta square. If, I add these two equations
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x1DUgD8MYSg_24.wav
|
|
both these terms 1 over M to 1 over N
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x1N00M-E0Gc_189.wav
|
|
it out that it is at the points where it is changing the values that is at 0 at 1 and
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x1UOO0FTQkA_358.wav
|
|
ok mind you c here c ah as matrix is ah you know its translation by minus z minus b of
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x1lmNkjI4OQ_220.wav
|
|
Yeah and this is kind of a slide show that is available on the net.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x2Lxt-KS_v4_132.wav
|
|
involved here and then1 ZA plus ZC will get cancelled here.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x2_dOFe9GLw_195.wav
|
|
temperature or elevated heat zone that is prevalent between the tool and the work piece.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x4xJLw8Vs4w_259.wav
|
|
We are applying a source VS having a source resistance RS.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x5sYcMFoCIs_509.wav
|
|
distribution and consumption.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x6937JZof3A_387.wav
|
|
wipes these are the other uses of the polyster.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x6L8wKhGfUw_59.wav
|
|
n2 let us take the first one namely n1 is 1, n2 is 1 and x, y is obviously the product
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x6OwyrODCVQ_125.wav
|
|
which is having a non-central F distribution on the degrees of freedom, and the non-centrality
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x6hH4ppKbqQ_133.wav
|
|
is how you can realize and, and with the help of this CPL.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x6iuqD94DOU_171.wav
|
|
effective value of r L, which we have talked two times at least in the two circuits.
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x6sj8dq1XJI_209.wav
|
|
transform pairs the original time function and its Fourier
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x783fNgQOfQ_29.wav
|
|
f s comma y where, y belongs to V, this is the total quantity of fluid that emerges from
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x8s2jJGCT8M_183.wav
|
|
between e and k simple, we will just use the result of free electron theory that is e is
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x9XJTRmtlMo_30.wav
|
|
uncertainty, effect-related uncertainty and timing-related uncertainty. So, considering
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x9lDM54CnyM_492.wav
|
|
other elements will be in the symmetry difference therefore the symmetric difference is a set
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/x9r-9X4VPhQ_46.wav
|
|
needs to be understood and how mistaken were understanding is about this concept,
|
/content/drive/MyDrive/IITKGP/dataset/tie_train_dataset/wav1/xA_txcLHRjk_30.wav
|
End of preview. Expand
in Data Studio
README.md exists but content is empty.
- Downloads last month
- 2